AP Physics 1 mock exam Free full practice test
A full-length practice test built from our exam-style questions on every unit of AP Physics 1. 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 180 minutes and work without notes. All questions use g = 9.8 m/s², as on the AP Physics 1 equation sheet. A calculator is allowed, as in the exam.
- 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: 48 exam-style questions
Hint
Dropped from rest means v0 = 0. Which equation links distance, time and acceleration?
Worked solution
- Take downward as positive, so a = g = 9.8 m/s² and v0 = 0.
- Δy = v0t + ½gt2 = 0 + ½(9.8)(2.5)2.
- Δy = 4.9 × 6.25 = 30.6 m.
Hint
Treat the vertical and horizontal motions separately. The vertical motion tells you the time in the air.
Worked solution
- Vertically the ball starts with zero velocity and falls 1.2 m: 1.2 = ½(9.8)t2.
- t = √(2 × 1.2 / 9.8) = 0.495 s.
- Horizontally the velocity stays at 3.0 m/s, so Δx = 3.0 × 0.495.
- Δx = 1.48 m.
Hint
Find the vertical component of the launch velocity first. The time up equals the time down.
Worked solution
- Vertical component: vy0 = 20 sin 30° = 10 m/s.
- Time to the top, where vy = 0: t = 10 / 9.8 = 1.02 s.
- The flight is symmetric on level ground, so the total time is 2 × 1.02 = 2.04 s, answer B.
- 1.02 s is only the time to the top, a common trap.
Hint
On a position-time graph, the slope is the velocity. What does a constant, negative slope mean?
Worked solution
- The slope of a position-time graph is the velocity.
- A straight line has a constant slope, so the velocity is constant and the acceleration is zero.
- The slope is negative, so the cart moves in the negative direction.
- The answer is B.
Hint
Write an expression for each car's position against time, then set them equal.
Worked solution
- Car A: xA = ½(2.0)t2 = t2.
- Car B: xB = 12t.
- Set them equal: t2 = 12t, so t(t − 12) = 0.
- t = 0 is the start, so A catches B at t = 12 s.
Hint
Take up as positive and the launch point as y = 0. Where is the ground?
Worked solution
- Take up as positive, so a = −9.8 m/s², and the ground is at y = −2.0 m.
- −2.0 = 15t − 4.9t2, so 4.9t2 − 15t − 2.0 = 0.
- Quadratic formula: t = [15 + √(225 + 39.2)] / 9.8 = (15 + 16.25) / 9.8.
- The positive root is t = 3.19 s.
Hint
Resolve the weight into components along and perpendicular to the ramp.
Worked solution
- Along the ramp the only force is the component of weight, mg sinθ.
- a = mg sinθ / m = g sinθ, so the mass cancels.
- a = 9.8 × sin 30° = 4.9 m/s², down the ramp.
Hint
Treat both masses and the string as one system. What is the net force that drives it?
Worked solution
- The net force on the system is the difference in weights: (5.0 − 3.0) × 9.8 = 19.6 N.
- The total mass being accelerated is 8.0 kg.
- a = 19.6 / 8.0 = 2.45 m/s².
Hint
Apply Newton's second law to the 3.0 kg mass alone. Which way does it accelerate?
Worked solution
- The 3.0 kg mass accelerates upward at 2.45 m/s².
- Newton's second law for it: T − mg = ma, so T = m(g + a).
- T = 3.0 × (9.8 + 2.45) = 36.8 N. Check: it lies between the two weights, 29.4 N and 49 N, as it must.
Hint
On a flat bend, friction is the only horizontal force, so it provides all of the centripetal force.
Worked solution
- The net force must point to the centre and equal mv2/r.
- F = 1200 × 152 / 50 = 1200 × 225 / 50.
- F = 5400 N, towards the centre of the bend.
Hint
At the lowest point, tension acts up and weight acts down. The net force must point up, towards the centre.
Worked solution
- Net force towards the centre (upward): T − mg = mv2/r.
- mv2/r = 0.50 × 16 / 0.80 = 10 N, and mg = 4.9 N.
- T = 4.9 + 10 = 14.9 N.
Hint
The force depends on 1/r2.
Worked solution
- Fg = Gm1m2/r2, an inverse-square law.
- Doubling r multiplies r2 by 4, so the force is divided by 4.
- The answer is B, one quarter.
Hint
Only the drop in height matters: energy lost as potential energy becomes kinetic energy.
Worked solution
- Conservation of energy: mgΔh = ½mv2, and the mass cancels.
- The car has dropped Δh = 25 − 10 = 15 m.
- v = √(2 × 9.8 × 15) = √294.
- v = 17.1 m/s.
Hint
The spring's elastic energy becomes the ball's kinetic energy.
Worked solution
- Elastic energy: ½kΔx2 = ½ × 400 × 0.102 = 2.0 J.
- Set 2.0 = ½ × 0.050 × v2, so v2 = 80.
- v = 8.94 m/s.
Hint
The work done by friction removes all the box's kinetic energy. Does the mass matter?
Worked solution
- Work-energy theorem: μmg d = ½mv2, so the mass cancels.
- μ = v2 / (2gd) = 25 / (2 × 9.8 × 3.0) = 25 / 58.8.
- μ = 0.425, about 0.43 (no units).
Hint
Compare their energies at the top of the cliff and at the ground.
Worked solution
- Both start with the same kinetic energy (same speed) and the same potential energy (same height).
- Both lose the same potential energy falling to the ground.
- So both arrive with the same kinetic energy, and the same speed. The answer is C. Only their times differ.
Hint
Compare the potential energy at the top with the kinetic energy at the bottom.
Worked solution
- Potential energy lost: mgh = 60 × 9.8 × 40 = 23,520 J.
- Kinetic energy gained: ½ × 60 × 202 = 12,000 J.
- Energy transferred by friction and air resistance: 23,520 − 12,000 = 11,520 J, about 11.5 kJ.
Hint
Kinetic energy depends on the square of the speed.
Worked solution
- K = ½mv2, so K is proportional to v2.
- Tripling v multiplies K by 32 = 9.
- The answer is C. This is why stopping distances grow so quickly with speed.
Hint
Total momentum before equals total momentum after.
Worked solution
- Momentum before: 2.0 × 3.0 + 0 = 6.0 kg·m/s.
- Afterwards they move together with mass 3.0 kg: 6.0 = 3.0v.
- v = 2.0 m/s.
Hint
Work out the total kinetic energy before and after.
Worked solution
- Before: ½ × 2.0 × 3.02 = 9.0 J.
- After: ½ × 3.0 × 2.02 = 6.0 J.
- Lost: 3.0 J, a third of the original kinetic energy.
Hint
The total momentum starts at zero, so it must stay zero.
Worked solution
- 0 = 50 × 1.4 + 70v, taking the 50 kg skater's direction as positive.
- v = −70 / 70 = −1.0 m/s.
- The 70 kg skater moves at 1.0 m/s in the opposite direction.
Hint
Both eggs stop from the same speed. What does that tell you about the impulse?
Worked solution
- Both eggs go from the same speed to rest, so the change in momentum, and the impulse, are the same.
- Impulse = FΔt. The pillow increases Δt, so the average force F is smaller.
- The answer is B, the same idea as crumple zones and airbags.
Hint
The area under a force-time graph is the impulse.
Worked solution
- Impulse = area of the triangle = ½ × 0.040 × 600 = 12 N·s.
- Impulse = Δp = mv − 0, so 12 = 0.40v.
- v = 30 m/s.
Hint
Write the momentum equation, and use the fact that in a head-on elastic collision the speed of approach equals the speed of separation.
Worked solution
- Momentum: 1.0(4.0) = 1.0v1 + 3.0v2.
- Elastic, head-on: v2 − v1 = 4.0, so v2 = v1 + 4.0.
- Substitute: 4.0 = v1 + 3v1 + 12, so 4v1 = −8.0.
- v1 = −2.0 m/s: the light cart bounces back. Check: v2 = 2.0 m/s, and kinetic energy 8 J before = 2 J + 6 J after.
Hint
For balance, the clockwise and anticlockwise torques about the pivot are equal.
Worked solution
- Torque balance: 30g × 2.0 = 40g × d, so g cancels.
- d = 60 / 40 = 1.5 m.
Hint
Take torques about the right-hand support, so its force has no torque.
Worked solution
- About the right support: the beam's weight acts 2.0 m away and the person 3.0 m away.
- Balance: FL × 4.0 = (20 × 9.8)(2.0) + (50 × 9.8)(3.0) = 392 + 1470.
- FL = 1862 / 4.0 = 466 N. Check: the right support gives 686 − 466 = 220 N, and the person is nearer the left, so the left force is larger, as expected.
Hint
Use Newton's second law for rotation.
Worked solution
- α = Στ / I = 6.0 / 0.50.
- α = 12 rad/s².
Hint
Find the rotational inertia and the torque separately.
Worked solution
- I = ½ × 2.0 × 0.102 = 0.010 kg·m².
- The string pulls tangentially at the rim: τ = 0.10 × 4.0 = 0.40 N·m.
- α = 0.40 / 0.010 = 40 rad/s².
Hint
Every point on the wheel has the same angular velocity ω.
Worked solution
- v = rω, and ω is the same for every point on the rigid wheel.
- The rim point is twice as far from the axle, so its linear speed is twice as large.
- The answer is B.
Hint
Write Newton's second law for the block and for the pulley, and link them with a = Rα.
Worked solution
- Block: mg − T = ma.
- Pulley: TR = Iα = (½MR2)(a/R), so T = ½Ma = 1.0a.
- Add the equations: mg = (m + ½M)a, so 9.8 = 2.0a.
- a = 4.9 m/s², less than g because some of the energy goes into turning the pulley.
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.
Hint
T depends on the square root of m.
Worked solution
- T = 2π√(m/k), so T is proportional to √m.
- Doubling m multiplies T by √2, about 1.41.
- The answer is B.
Hint
At equilibrium, all of the spring energy ½kA2 has become kinetic energy.
Worked solution
- ½kA2 = ½mvmax2, so vmax = A√(k/m).
- vmax = 0.20 × √(50 / 0.50) = 0.20 × 10.
- vmax = 2.0 m/s.
Hint
At the amplitude the mass is momentarily at rest, so all the energy is stored in the spring.
Worked solution
- E = ½kA2 = ½ × 50 × 0.202.
- E = 1.0 J. Check: ½ × 0.50 × 2.02 = 1.0 J too.
Hint
T depends on 1/√g.
Worked solution
- T = 2π√(L/g), so T is proportional to 1/√g.
- Dividing g by 6 multiplies T by √6, about 2.45.
- The answer is B: the clock runs slow.
Hint
Rearrange T = 2π√(L/g) for L.
Worked solution
- Square both sides: T2 = 4π2L/g, so L = gT2 / 4π2.
- L = 9.8 × 1.52 / 39.48 = 22.05 / 39.48.
- L = 0.559 m, about 56 cm.
Hint
You do not need the mass or k separately: the stretch tells you m/k.
Worked solution
- At equilibrium kx = mg, so m/k = x/g = 0.049 / 9.8 = 0.0050 s².
- T = 2π√(m/k) = 2π√0.0050.
- T = 0.444 s.
Hint
The buoyant force equals the weight of the water displaced.
Worked solution
- Fb = ρwaterVg = 1000 × 0.0020 × 9.8.
- Fb = 19.6 N, whatever the object is made of.
Hint
Set the buoyant force equal to the weight, and write both in terms of densities and volumes.
Worked solution
- Floating: ρwaterVunderg = ρwoodVtotalg.
- Vunder / Vtotal = ρwood / ρwater = 600 / 1000.
- Fraction under water = 0.60.
Hint
In a horizontal pipe the ρgy terms cancel in Bernoulli's equation.
Worked solution
- P1 + ½ρv12 = P2 + ½ρv22.
- P1 − P2 = ½ × 1000 × (6.02 − 2.02) = 500 × 32.
- P1 − P2 = 16,000 Pa. Faster flow, lower pressure.
Hint
Apply Bernoulli's equation between the surface and the hole. Both are at atmospheric pressure, and the surface barely moves.
Worked solution
- The pressure terms cancel and the surface speed is about zero, so ρgh = ½ρv2.
- v = √(2gh) = √(2 × 9.8 × 1.8) = √35.28.
- v = 5.94 m/s, the same speed as an object falling 1.8 m.
Hint
The buoyant force must still equal the ship's weight. How much denser water must it displace for that?
Worked solution
- Floating, the buoyant force equals the weight in both cases, so the buoyant force does not change.
- Fb = ρVg: with larger ρ, a smaller volume V is needed.
- The ship displaces less water, so it rises: B.
Hint
The loss in weight is the buoyant force, which tells you the rock's volume.
Worked solution
- Buoyant force = 30 − 20 = 10 N = ρwaterVg.
- The rock's weight is ρrockVg = 30 N.
- Divide: ρrock / ρwater = 30 / 10 = 3.0.
- ρrock = 3000 kg/m³.
Section II: 4 free-response questions
Free-response question 1: Kinematics
Mathematical routines style · 6 points · about 20 minutes
A student throws a ball horizontally at 8.0 m/s from the top of a building of height H = 20 m. Air resistance is negligible.
- (a) Derive an expression for the time t the ball takes to reach the ground, in terms of H and physical constants.
- (b) Calculate the horizontal distance from the base of the building to where the ball lands.
- (c) A second ball is thrown horizontally from the same point at 16 m/s. Compare its time in the air and its landing distance with the first ball's. Justify your answers.
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)
Vertically the ball starts from rest: H = ½gt2, so t = √(2H/g).
Part (b)
t = √(2 × 20 / 9.8) = 2.02 s. Horizontal velocity is constant, so d = 8.0 × 2.02 = 16.2 m.
Part (c)
The time is the same, because the vertical motion (start at rest vertically, fall H with acceleration g) does not depend on the horizontal velocity. The distance doubles, because d = vxt and vx doubles while t stays the same.
Your mark: 0 of 6
Free-response question 2: Work, energy and power
Qualitative/quantitative translation style · 6 points · about 22 minutes
A block of mass m is released from rest at height h on a frictionless curved ramp. At the bottom it slides onto a rough horizontal surface with coefficient of kinetic friction μ, and comes to rest after sliding a distance d along it.
- (a) Derive an expression for d in terms of h and μ.
- (b) A student claims that a heavier block released from the same height would slide further, because it has more energy at the bottom. Explain whether the student is correct.
- (c) The block is released from height 2h instead. By what factor does d change? Justify your answer using part (a).
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)
The potential energy mgh is all removed by the work done by friction, μmg d. So mgh = μmg d, which gives d = h / μ.
Part (b)
The student is wrong. A heavier block does have more kinetic energy at the bottom, but the friction force μmg is larger by the same factor. The mass cancels, so d = h/μ is the same for any mass.
Part (c)
d = h/μ is directly proportional to h, so doubling the height doubles the stopping distance.
Your mark: 0 of 6
Free-response question 3: Energy and momentum of rotating systems
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
Free-response question 4: Fluids
Translation between representations style · 5 points · about 20 minutes
A block hangs from a spring scale. The scale reads W in air. The block is then lowered slowly into a beaker of water until it is completely under water, and then lowered further without touching the bottom.
- (a) Sketch, or describe, a graph of the scale reading against the depth of the block's bottom face below the water surface.
- (b) Derive an expression for the density of the block, in terms of W, the fully submerged reading W′, and the density of water ρw.
- (c) W = 12 N and W′ = 7.5 N. Calculate the density of the block.
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)
The reading starts at W. As the block goes under, the buoyant force grows in proportion to the volume under water, so the reading falls in a straight line. Once the block is fully under water, the displaced volume stops changing, so the reading stays constant at a lower value W′.
Part (b)
Buoyant force when fully submerged: W − W′ = ρwVg. Weight: W = ρVg. Dividing gives ρ = ρwW / (W − W′).
Part (c)
ρ = 1000 × 12 / 4.5 = 2670 kg/m³.
Your mark: 0 of 5
After the mock
Note every question you missed and its unit, then go back to that unit's practice page: all AP Physics 1 units. Then try the real thing with official AP Physics 1 past papers.