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How does a capacitor store charge and energy, and how does it discharge through a resistor?

Capacitors: capacitance and the farad, capacitors in series and parallel, the energy stored in a capacitor, and the exponential charge and discharge through a resistor with the time constant.

A focused answer to the OCR H556 capacitors content, covering capacitance and the farad, combining capacitors in series and parallel, the energy stored in a capacitor, and the exponential charging and discharging of a capacitor through a resistor with the time constant.

Generated by Claude Opus 4.812 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

OCR wants you to define capacitance and the farad, use Q=CVQ = CV, combine capacitors in series and parallel, find the energy stored in a capacitor, and analyse the exponential charge and discharge of a capacitor through a resistor using the time constant.

The answer

Capacitance and the farad

Capacitors in series and parallel

Energy stored

Charging and discharging through a resistor

Examples in context

Capacitors smooth the output of rectified power supplies, provide the energy burst in a camera flash and a defibrillator, and store charge in the memory cells of computers. The time constant sets the timing in flashing-indicator and timer circuits, and the slow discharge of a capacitor through a resistor is used in touchscreens and in audio filters that block or pass particular frequencies. Supercapacitors store large amounts of charge for rapid energy delivery in vehicles.

Try this

Q1. Define capacitance and state its unit. [2 marks]

  • Cue. The charge stored per unit potential difference, C=QVC = \frac{Q}{V}, in farads.

Q2. Two 4.0 μF4.0\ \mu\text{F} capacitors are connected in parallel. Find the total capacitance. [1 mark]

  • Cue. In parallel, C=4.0+4.0=8.0 μFC = 4.0 + 4.0 = 8.0\ \mu\text{F}.

Q3. A 1000 μF1000\ \mu\text{F} capacitor discharges through a 2.0 kΩ2.0\ \text{k}\Omega resistor. Find the time constant. [2 marks]

  • Cue. τ=RC=(2.0×103)(1000×106)=2.0 s\tau = RC = (2.0 \times 10^{3})(1000 \times 10^{-6}) = 2.0\ \text{s}.

Exam-style practice questions

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

OCR 20184 marksA 2200 μF2200\ \mu\text{F} capacitor is charged to 12 V12\ \text{V}. Calculate the charge stored and the energy stored.
Show worked answer →

Charge: Q=CV=(2200×106)(12)=2.64×102 CQ = CV = (2200 \times 10^{-6})(12) = 2.64 \times 10^{-2}\ \text{C}, about 0.026 C0.026\ \text{C}.

Energy: E=12CV2=12(2200×106)(12)2=12(2200×106)(144)=0.16 JE = \frac{1}{2}CV^2 = \frac{1}{2}(2200 \times 10^{-6})(12)^2 = \frac{1}{2}(2200 \times 10^{-6})(144) = 0.16\ \text{J}.

Markers reward Q=CVQ = CV giving about 0.026 C0.026\ \text{C}, and E=12CV2E = \frac{1}{2}CV^2 giving about 0.16 J0.16\ \text{J}. The half is essential, since energy is the area under the charge-voltage graph.

OCR 20215 marksA 470 μF470\ \mu\text{F} capacitor charged to 9.0 V9.0\ \text{V} is discharged through a 10 kΩ10\ \text{k}\Omega resistor. Calculate the time constant and the potential difference across the capacitor 3.0 s3.0\ \text{s} after discharge begins.
Show worked answer →

Time constant: τ=RC=(10×103)(470×106)=4.7 s\tau = RC = (10 \times 10^{3})(470 \times 10^{-6}) = 4.7\ \text{s}.

Discharge: V=V0et/RC=9.0e3.0/4.7V = V_0 e^{-t/RC} = 9.0\, e^{-3.0/4.7}.

Exponent: 3.04.7=0.638\frac{-3.0}{4.7} = -0.638, so e0.638=0.528e^{-0.638} = 0.528.

V=9.0×0.528=4.8 VV = 9.0 \times 0.528 = 4.8\ \text{V}.

Markers reward τ=RC=4.7 s\tau = RC = 4.7\ \text{s}, the exponential form V=V0et/RCV = V_0 e^{-t/RC}, and the value about 4.8 V4.8\ \text{V}.

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