AP Physics C: E&M mock exam Free full practice test
A full-length practice test built from our exam-style questions on every unit of AP Physics C: E&M. 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. Constants as on the AP reference sheet: k = 9.0 × 109 N·m²/C², ε0 = 8.85 × 10−12 C²/(N·m²), μ0 = 4π × 10−7 T·m/A, e = 1.6 × 10−19 C. You can type answers like 3.6e5 or 3.6x10^5.
- 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: 30 exam-style questions
Hint
Gauss's law: the flux depends only on the charge enclosed.
Worked solution
- Φ = qenc/ε0.
- = 5.0 × 10−9/8.85 × 10−12.
- Φ = 565 N·m²/C, whatever the shape of the surface.
Hint
Use a cylindrical Gaussian surface around the wire.
Worked solution
- Gauss's law with a cylinder of radius r and length L: E(2πrL) = λL/ε0.
- E = λ/(2πε0r) = 2.0 × 10−6/(2π × 8.85 × 10−12 × 0.10).
- E = 3.60 × 105 N/C.
Hint
Draw a Gaussian sphere inside the shell. How much charge does it enclose?
Worked solution
- A Gaussian sphere inside the shell encloses no charge.
- By symmetry E is the same all over that sphere, so E × 4πr2 = 0.
- So E = 0 everywhere inside: A.
Hint
Inside a uniform sphere, only the charge within radius r counts, and it grows as r3.
Worked solution
- Enclosed charge: Q(r/R)3. So E = kQr/R3.
- E = 9.0 × 109 × 8.0 × 10−9 × 0.10/0.203 = 7.2/0.008.
- E = 900 N/C.
Hint
Use a Gaussian “pillbox” through the sheet.
Worked solution
- The flux leaves through both faces: E × 2A = σA/ε0.
- E = σ/(2ε0) = 1.77 × 10−9/(1.77 × 10−11).
- E = 100 N/C, independent of distance.
Hint
Ex = −dV/dx.
Worked solution
- dV/dx = 8x.
- Ex = −8 × 2 = −16 V/m: the field points in the negative x direction.
Hint
The energy gained is eΔV, and it becomes kinetic energy.
Worked solution
- eΔV = ½mv2, so v = √(2eΔV/m).
- v = √(2 × 1.6 × 10−19 × 100/9.11 × 10−31).
- v = 5.93 × 106 m/s.
Hint
U = kq1q2/r, keeping the signs.
Worked solution
- U = 9.0 × 109 × (3.0 × 10−6)(−2.0 × 10−6)/0.20.
- U = −0.27 J. Negative: the pair is bound.
Hint
Potential is a scalar: add the four contributions.
Worked solution
- Each charge is half a diagonal away: 0.20/√2 = 0.1414 m.
- Each gives kq/r = 9.0/0.1414 = 63.6 V.
- Total = 4 × 63.6 = 255 V (while the field at the centre is zero).
Hint
In a uniform field, |ΔV| = Ed.
Worked solution
- |ΔV| = 300 × 0.050.
- = 15 V, lower in the direction of the field.
Hint
C = ε0A/d, then convert to pF.
Worked solution
- C = 8.85 × 10−12 × 0.010/1.0 × 10−3.
- C = 8.85 × 10−11 F.
- = 88.5 pF.
Hint
In series, the reciprocals add.
Worked solution
- 1/C = 1/3 + 1/6 = 1/2.
- C = 2.0 μF, smaller than either one.
Hint
In parallel, capacitances simply add.
Worked solution
- C = 3.0 + 6.0 = 9.0 μF.
Hint
The battery fixes the voltage.
Worked solution
- The dielectric multiplies C by κ.
- The battery holds V constant, so Q = CV increases.
- The answer is A. (Disconnected, Q would stay fixed and V would fall.)
Hint
The sphere's potential is kQ/R, so C = Q/V.
Worked solution
- V = kQ/R, so C = R/k = 4πε0R.
- C = 4π × 8.85 × 10−12 × 0.10 = 1.11 × 10−11 F.
- = 11.1 pF.
Hint
P = I2R.
Worked solution
- P = 2.02 × 6.0 = 24 W.
Hint
τ = RC, in base units.
Worked solution
- τ = 2000 × 50 × 10−6.
- τ = 0.10 s.
Hint
After one time constant, the capacitor has reached 1 − e−1 of its final value.
Worked solution
- VC = 12(1 − e−1) = 12 × 0.632.
- VC = 7.59 V.
Hint
Find the current first, using the total resistance.
Worked solution
- I = 12/(5.5 + 0.50) = 2.0 A.
- Terminal voltage = ε − Ir = 12 − 2.0 × 0.50.
- = 11 V.
Hint
Voltage falls as e−t/RC. Half the voltage means one “half-life”.
Worked solution
- RC = 104 × 10−4 = 1.0 s.
- 4.5 = 9.0e−t/RC, so t = RC ln 2.
- t = 0.693 s.
Hint
The magnetic force provides the centripetal force: qvB = mv2/r.
Worked solution
- r = mv/(qB).
- r = 9.11 × 10−31 × 1.0 × 106/(1.6 × 10−19 × 0.010).
- r = 5.69 × 10−4 m.
Hint
One wire sits in the other's field: F/L = I2B1.
Worked solution
- F/L = μ0I1I2/(2πd).
- = 4π × 10−7 × 25/(2π × 0.10).
- F/L = 5.0 × 10−5 N/m, attractive if the currents are in the same direction.
Hint
B = μ0nI.
Worked solution
- B = 4π × 10−7 × 1000 × 2.0.
- B = 2.51 × 10−3 T.
Hint
F = ILB.
Worked solution
- F = 3.0 × 0.20 × 0.40 = 0.24 N.
Hint
Apply Ampère's law to a circle of radius r inside the wire.
Worked solution
- The enclosed current is I(r/R)2.
- B(2πr) = μ0I r2/R2, so B = μ0Ir/(2πR2).
- B grows in proportion to r: C.
Hint
Faraday's law, with N turns.
Worked solution
- |ε| = NΔΦ/Δt = 100 × 0.020/0.10.
- = 20 V.
Hint
ε = L dI/dt (magnitude).
Worked solution
- |ε| = 0.50 × 4.0 = 2.0 V.
Hint
U = ½LI2.
Worked solution
- U = ½ × 0.20 × 3.02 = 0.90 J.
Hint
τ = L/R.
Worked solution
- τ = 0.30/6.0 = 0.050 s.
Hint
The current rises towards ε/R as 1 − e−t/τ.
Worked solution
- Final current: 12/4.0 = 3.0 A.
- I(τ) = 3.0(1 − e−1) = 3.0 × 0.632.
- I = 1.90 A.
Section II: 4 free-response questions
Free-response question 1: Electric charges, fields and Gauss's law
Mathematical routines style · 6 points · about 20 minutes
A solid insulating sphere of radius R has total charge Q spread uniformly through its volume.
- (a) Use Gauss's law to derive the electric field at a distance r < R from the centre.
- (b) Derive the field for r > R.
- (c) Sketch or describe the graph of E against r from r = 0 to r = 3R.
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)
Enclosed charge Q(r/R)3. E(4πr2) = Qr3/(ε0R3), so E = Qr/(4πε0R3).
Part (b)
All the charge is enclosed: E = Q/(4πε0r2).
Part (c)
E rises linearly from 0 at the centre to a maximum at r = R, then falls as 1/r2.
Your mark: 0 of 6
Free-response question 2: Conductors and capacitors
Qualitative/quantitative translation style · 6 points · about 20 minutes
A parallel-plate capacitor with plate area A and separation d is charged by a battery of voltage V0, and then disconnected. The plates are then pulled apart to separation 2d.
- (a) Derive the capacitance of the original capacitor using Gauss's law.
- (b) After the plates are pulled apart, state whether Q, C, V and the stored energy increase, decrease or stay the same. Justify each.
- (c) Where does the extra stored energy come from?
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)
Field between the plates E = σ/ε0 = Q/(ε0A). V = Ed = Qd/(ε0A), so C = Q/V = ε0A/d.
Part (b)
Q stays the same (disconnected). C halves (C ∝ 1/d). V = Q/C doubles. U = Q2/(2C) doubles.
Part (c)
From the work done by whoever pulls the plates apart against their mutual attraction.
Your mark: 0 of 6
Free-response question 3: Electric circuits
Mathematical routines style · 7 points · about 20 minutes
An uncharged capacitor C is connected in series with a resistor R, a battery of emf ε and a switch. The switch is closed at t = 0.
- (a) Use Kirchhoff's loop rule to write a differential equation for the charge q on the capacitor.
- (b) Solve it to find q(t).
- (c) Find the current immediately after the switch closes, and after a long time.
- (d) Show that the energy dissipated in the resistor while charging equals the energy finally stored in the capacitor.
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)
ε − R(dq/dt) − q/C = 0.
Part (b)
Separating: dq/(Cε − q) = dt/(RC), giving q(t) = Cε(1 − e−t/RC).
Part (c)
At t = 0 the capacitor acts like a wire: I = ε/R. After a long time it is fully charged: I = 0.
Part (d)
The battery supplies Qε = Cε2; the capacitor stores ½Cε2; so the resistor dissipates the other ½Cε2.
Your mark: 0 of 7
Free-response question 4: Electromagnetic induction
Qualitative/quantitative translation style · 7 points · about 20 minutes
A conducting rod of length L slides at constant speed v along two parallel rails joined by a resistor R. A uniform field B points into the page, at right angles to the rails.
- (a) Derive the emf induced in the circuit.
- (b) Find the current, and state its direction using Lenz's law.
- (c) Find the external force needed to keep the rod moving at constant speed.
- (d) Show that the mechanical power supplied equals the electrical power dissipated in R.
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 area grows at Lv per second, so dΦ/dt = BLv and ε = BLv.
Part (b)
I = BLv/R. The flux into the page is increasing, so the induced current is anticlockwise, making a field out of the page.
Part (c)
The magnetic force on the rod is ILB = B2L2v/R, opposing the motion, so the pulling force must equal it.
Part (d)
Fv = B2L2v2/R, and I2R = (BLv/R)2R = B2L2v2/R. They are equal: energy is conserved.
Your mark: 0 of 7
After the mock
Note every question you missed and its unit, then go back to that unit's practice page: all AP Physics C: E&M units. Then try the real thing with official AP Physics C: E&M past papers.