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Lesson 2 of 4 35 min

Capacitors and Inductors

Energy storage in an electric field and a magnetic field, the formulas that describe each, and their complementary DC and AC behaviour.

In this lesson
  • Calculate stored charge and energy in a capacitor
  • Calculate the voltage induced by a changing inductor current
  • Explain why capacitors block steady DC and inductors pass it

A capacitor stores energy in an electric field between two conductors separated by a dielectric. An inductor stores energy in a magnetic field created by current through a coil. Their behaviour is complementary: a capacitor opposes a change of voltage, while an inductor opposes a change of current.

Capacitance

C = Q ÷ V
Capacitance C in farads equals stored charge Q in coulombs divided by voltage V in volts.
E = ½ × C × V²
Energy stored in a capacitor, in joules.
Worked example

Charge and energy in a capacitor

Problem. A 100 µF capacitor is charged to 50 V. Find the stored charge and energy.

Solution. Q = C × V = 100 × 10⁻⁶ × 50 = 5 × 10⁻³ C = 5 mC. E = ½ × 100 × 10⁻⁶ × 50² = 0.5 × 100 × 10⁻⁶ × 2500 = 0.125 J.

Inductance

V = L × ΔI ÷ Δt
Induced voltage across an inductor; L in henries, ΔI in amperes and Δt in seconds.
E = ½ × L × I²
Energy stored in an inductor, in joules.
Worked example

Voltage across an inductor

Problem. The current through a 10 mH inductor rises from 0 A to 2 A in 5 ms. What average voltage appears across it?

Solution. ΔI/Δt = 2 ÷ 0.005 = 400 A/s. V = L × ΔI/Δt = 0.010 × 400 = 4 V.

  • A capacitor blocks steady DC after charging and passes changing signals more readily at higher frequency.
  • An inductor passes steady DC and opposes changes of current.
  • Both components store energy and can deliver it after the supply is removed.
  • Electrolytic capacitors are polarised and must be connected with the correct polarity.
A charged capacitor can remain dangerous after the supply is switched off. Discharge it through an appropriate resistor and verify the voltage before touching the terminals.
Key points.
  • C = Q/V and E = ½CV² describe a capacitor.
  • V = L di/dt and E = ½LI² describe an inductor.
  • Capacitors oppose voltage change; inductors oppose current change.
  • Both store energy that persists after isolation.
Practice

Worked example

A 10 mH inductor carrying 2 A stores E = ½ × 0.010 × 2² = 0.02 J. That energy must be absorbed by a flyback path when the current is interrupted.

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