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AP® Physics C: Electricity and Magnetism · Unit 13 · Topic 13.6

Circuits with Capacitors and Inductors (LC Circuits): Revision Notes (Physics C: E&M 13.6)

One-page recap of LC circuits for the calculus-based course: energy exchange, maximum current, the simple harmonic equation for charge, ω = 1/√(LC) and the phase of q and I.

Short on time? This page is the recap. For the derivations, Figure 1 and the worked examples, use the full study guide. This topic is in the calculus-based course.

Recap

  • A charged capacitor connected across an inductor (no resistor) oscillates: energy moves between the electric field and the magnetic field.
  • The total energy is constant, so the maximum current follows from energy conservation alone.
  • The loop rule, q/C + L dI/dt = 0 with I = dq/dt, gives the simple harmonic equation for q.
  • The period depends only on L and C, not on the starting charge.
  • Mass–spring analogy: q ↔ x, I ↔ v, L ↔ m, 1/C ↔ k.
  • If the oscillation starts from an inductor current I₀ with the capacitor empty, use q = Q_max sin ωt and I = I₀ cos ωt instead; the capacitor’s voltage can then be much larger than the emf that first set up I₀.

Key relationships

Quantity Result
Energy (constant) q²/(2C) + ½LI² = Q₀²/(2C)
Maximum current I_max = Q₀/√(LC) = ωQ₀
Maximum charge from a starting current I₀ Q_max = I₀√(LC)
Differential equation d²q/dt² = −q/(LC)
Angular frequency ω = 1/√(LC) (rad/s)
Period and frequency T = 2π√(LC); f = 1/(2π√(LC))
Starting fully charged q = Q₀ cos ωt; I = −ωQ₀ sin ωt
Energies U_C = (Q₀²/2C)cos² ωt; U_L = (Q₀²/2C)sin² ωt; each repeats every T/2
Charged by a battery ℰ Q₀ = Cℰ; I_max = ℰ√(C/L)

Assumptions behind the results

  • No resistance anywhere, so no energy is dissipated.
  • A single capacitor (or equivalent capacitance) and a single inductor.
  • The switch connects the elements instantly and adds no resistance.

Mistakes to avoid

  1. Putting I_max at full charge. The current is zero when |q| is greatest.
  2. Confusing ω and f. f = ω/(2π).
  3. Thinking the period depends on Q₀. It does not.
  4. Wrong energy period. U_C and U_L repeat every T/2.
  5. Factor-of-change slips. Decide whether Q₀ or the voltage is fixed before scaling.
  6. Using √(L/C) as a time. Only √(LC) is in seconds.

Quick self-check

  1. L = 0.10 H and C = 10 μF. What is ω? (1.0 × 10³ rad/s)
  2. For that circuit, what is T? (6.3 ms)
  3. Q₀ = 2.0 × 10⁻⁴ C in the same circuit. What is I_max? (0.20 A)
  4. The capacitor starts fully charged. When is all the energy first in the inductor? (At T/4)
  5. The same circuit at T/8: what fraction of the energy is in the capacitor? (One half)

Next: practice questions.

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