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EnglandPhysicsSyllabus dot point

How does the charge on a capacitor change with time as it charges or discharges through a resistor?

Exponential charge and discharge of a capacitor through a resistor, the time constant, and graphical and logarithmic analysis of the decay.

A focused answer to AQA A-Level Physics 3.7.4.4, covering the exponential charge and discharge of a capacitor through a resistor, the time constant RC, half-life of decay, and analysis using log-linear graphs.

Generated by Claude Opus 4.810 min answer

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

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  1. What this dot point is asking
  2. Discharging a capacitor
  3. The time constant
  4. Half-life of the decay
  5. Charging a capacitor
  6. Analysing decay with logarithms
  7. Try this

What this dot point is asking

AQA specification point 3.7.4.4 wants you to describe and use the exponential charge and discharge of a capacitor through a resistor, define and use the time constant, and analyse decay graphically, including using log-linear plots to find the time constant.

Discharging a capacitor

When a charged capacitor discharges through a resistor, the rate of loss of charge is proportional to the charge remaining. This is because the discharge current is I=VR=QRCI = \dfrac{V}{R} = \dfrac{Q}{RC}, and a current is a rate of loss of charge, so dQdt=QRC\dfrac{\mathrm{d}Q}{\mathrm{d}t} = -\dfrac{Q}{RC}. Any quantity whose rate of change is proportional to itself decays exponentially.

The voltage and current decay together because V=QCV = \dfrac{Q}{C} and I=VRI = \dfrac{V}{R} are both proportional to QQ at every instant.

The time constant

After one time constant the quantity has fallen to 37 percent; after two, to 13.5 percent; after about five time constants the capacitor is effectively fully discharged (under 1 percent remaining). A larger RR or CC slows the discharge, because a larger resistance restricts the current and a larger capacitance stores more charge to lose.

Half-life of the decay

This is the time for the charge to halve, directly analogous to radioactive decay, where the activity halves every half-life. The decay constant of the capacitor circuit is 1RC\dfrac{1}{RC}.

Charging a capacitor

Analysing decay with logarithms

Taking natural logs of the discharge equation gives a straight line:

A graph of lnQ\ln Q against tt has gradient 1RC-\dfrac{1}{RC}, so the time constant is found as the negative reciprocal of the gradient. Linearising in this way is the standard exam method because a straight-line fit is more reliable than reading a curve.

Try this

Q1. Define the time constant of a capacitor-resistor circuit. [1 mark]

  • Cue. The time for the charge to fall to 1e\dfrac{1}{e} (about 37 percent) of its initial value, τ=RC\tau = RC.

Q2. A capacitor discharges with a time constant of 4.0 s4.0 \text{ s}. What fraction of the initial charge remains after 4.0 s4.0 \text{ s}? [1 mark]

  • Cue. e10.37e^{-1} \approx 0.37, so about 37 percent remains.

Q3. State how the half-life of a capacitor discharge relates to the time constant. [1 mark]

  • Cue. T1/2=0.69RC=ln2×τT_{1/2} = 0.69RC = \ln 2 \times \tau.

Exam-style practice questions

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

AQA 20195 marksA 470 μF470 \text{ }\mu\text{F} capacitor is charged to 6.0 V6.0 \text{ V} and then discharged through a 22 kΩ22 \text{ k}\Omega resistor. Calculate the time constant and the potential difference across the capacitor 20 s20 \text{ s} after the discharge begins.
Show worked answer →

The time constant is τ=RC=(22×103)(470×106)=10.3 s\tau = RC = (22 \times 10^3)(470 \times 10^{-6}) = 10.3 \text{ s}.

The discharge follows V=V0et/RCV = V_0 e^{-t/RC}, so V=6.0×e20/10.3=6.0×e1.94V = 6.0 \times e^{-20/10.3} = 6.0 \times e^{-1.94}.

Since e1.94=0.144e^{-1.94} = 0.144, V=6.0×0.144=0.86 VV = 6.0 \times 0.144 = 0.86 \text{ V}.

Markers reward converting to SI base units, the correct time constant, and substituting into the exponential decay equation. A common error is leaving the capacitance in microfarads.

AQA 20214 marksA student discharges a capacitor through a fixed resistor and records the charge at intervals. Explain how plotting the natural logarithm of charge against time can be used to find the time constant of the circuit.
Show worked answer →

Taking natural logarithms of Q=Q0et/RCQ = Q_0 e^{-t/RC} gives lnQ=lnQ0tRC\ln Q = \ln Q_0 - \dfrac{t}{RC}, which is a straight line of the form y=c+mxy = c + mx with lnQ\ln Q on the vertical axis and tt on the horizontal axis.

The gradient of the line is 1RC-\dfrac{1}{RC}, so the time constant is the negative reciprocal of the gradient, RC=1gradientRC = -\dfrac{1}{\text{gradient}}.

Using a logarithmic plot turns the exponential into a straight line, which is easier to fit and reduces the effect of random scatter than reading a single point off a curve.

Markers reward taking logs to linearise, identifying the gradient as 1RC-\dfrac{1}{RC}, and extracting the time constant from the gradient.

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