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How do capacitors and inductors store energy, and how do they charge and discharge through a resistor?

Capacitors and inductors: capacitance and stored energy, the RC time constant and exponential charge and discharge, inductance and stored energy, and combining capacitors in series and parallel.

An Eduqas A-Level Electronics answer on capacitors and inductors: capacitance and the energy stored in a capacitor, the RC time constant and exponential charge and discharge, inductance and the energy stored in an inductor, and how capacitors combine in series and parallel (the reverse of resistors).

Generated by Claude Opus 4.814 min answer

Reviewed by: AI editorial process; not yet individually human-reviewed

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  1. What this dot point is asking
  2. The answer
  3. Examples in context
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What this dot point is asking

Eduqas wants you to define capacitance and the energy stored in a capacitor, use the RC time constant with the exponential charge and discharge equations, define inductance and the energy stored in an inductor, and combine capacitors in series and parallel. These energy-storing components set timing, smooth supplies and shape signals throughout the course.

The answer

Capacitance and stored energy

The RC time constant and exponential charge and discharge

Inductance and stored energy

Combining capacitors

Examples in context

Capacitors set the timing of 555 astables and monostables, smooth the rectified output of a mains power supply, couple audio between amplifier stages, and decouple the supply pins of logic chips. The 5-time-constant rule decides how long a timing circuit takes to settle and how big a smoothing capacitor a power supply needs. Inductors and capacitors together tune radio receivers and form the energy-transfer element of switch-mode supplies.

Try this

Q1. A 220 μF220\ \mu\text{F} capacitor is charged to 5.0 V5.0\ \text{V}. Find the charge stored. [2 marks]

  • Cue. Q=CV=220×106×5.0=1.1×103 CQ = CV = 220 \times 10^{-6} \times 5.0 = 1.1 \times 10^{-3}\ \text{C}.

Q2. A 10 μF10\ \mu\text{F} capacitor discharges through a 100 kΩ100\ \text{k}\Omega resistor. Find the time constant. [2 marks]

  • Cue. τ=RC=100000×10×106=1.0 s\tau = RC = 100000 \times 10 \times 10^{-6} = 1.0\ \text{s}.

Q3. Two 4.7 μF4.7\ \mu\text{F} capacitors are connected in parallel. Find the total capacitance. [1 mark]

  • Cue. C=4.7+4.7=9.4 μFC = 4.7 + 4.7 = 9.4\ \mu\text{F} (parallel adds).

Exam-style practice questions

Practice questions written in the style of WJEC Eduqas exam questions on this dot point, with worked answer explainers. The year tag is the paper they imitate, not the source.

Eduqas 20196 marksA 470 μF470\ \mu\text{F} capacitor is charged to 9.0 V9.0\ \text{V} and then discharged through a 22 kΩ22\ \text{k}\Omega resistor. Calculate the time constant, the energy initially stored, and the voltage across the capacitor after 20 s20\ \text{s}.
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Time constant (up to 2 marks): τ=RC=22000×470×106=10.3 s\tau = RC = 22000 \times 470 \times 10^{-6} = 10.3\ \text{s}.

Energy stored (up to 2 marks): E=12CV2=12×470×106×9.02=12×470×106×81=1.9×102 JE = \frac{1}{2}CV^2 = \frac{1}{2} \times 470 \times 10^{-6} \times 9.0^2 = \frac{1}{2} \times 470 \times 10^{-6} \times 81 = 1.9 \times 10^{-2}\ \text{J}.

Voltage after 20 s20\ \text{s} (up to 2 marks): V=V0et/RC=9.0e20/10.3=9.0e1.94=9.0×0.144=1.3 VV = V_0 e^{-t/RC} = 9.0\, e^{-20/10.3} = 9.0\, e^{-1.94} = 9.0 \times 0.144 = 1.3\ \text{V}.

Markers reward τ=10.3 s\tau = 10.3\ \text{s}, E=1.9×102 JE = 1.9 \times 10^{-2}\ \text{J}, and the discharge value 1.3 V1.3\ \text{V} using V=V0et/RCV = V_0 e^{-t/RC}.

Eduqas 20224 marksExplain what the time constant of an RC circuit represents, and state how many time constants are needed for a capacitor to be considered fully discharged.
Show worked answer →

Meaning (up to 3 marks): the time constant τ=RC\tau = RC is the time taken for the charge (or voltage, or current) on a discharging capacitor to fall to 1e\frac{1}{e}, about 37 per cent, of its initial value. Equivalently it is the time to rise to about 63 per cent of the final value when charging. A larger resistance or capacitance gives a slower response.

Fully discharged (up to 1 mark): after about 5 time constants the capacitor has fallen to under 1 per cent of its initial value and is treated as fully discharged.

Markers reward the 1e\frac{1}{e} (37 per cent) definition, the link to RCRC, and the "5 time constants" rule of thumb.

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