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9702 · 19.1

Capacitors and capacitance — practice questions

Practice and worked examples for 9702 Capacitors and capacitance. Short previews only — attempt the full question in MarkScheme against the official scheme.

Worked example 1

Two capacitors, C1=4.0μFC_1 = 4.0 \mu\text{F} and C2=6.0μFC_2 = 6.0 \mu\text{F}, are connected to a 12 V12 \text{ V} power supply. Calculate the total capacitance and the total charge stored when they are connected: (a) in series (b) in parallel

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(a) In Series:

  1. Use the series capacitance formula: 1Ctotal=1C1+1C2\frac{1}{C_{total}} = \frac{1}{C_1} + \frac{1}{C_2} 1Ctotal=14.0×106 F+16.0×106 F\frac{1}{C_{total}} = \frac{1}{4.0 \times 10^{-6} \text{ F}} + \frac{1}{6.0 \times 10^{-6} \text{ F}} 1Ctotal=(2.5×105+1.667×105) F1=4.167×105 F1\frac{1}{C_{total}} = (2.5 \times 10^5 + 1.667 \times 10^5) \text{ F}^{-1} = 4.167 \times 10^5 \text{ F}^{-1} Ctotal=14.167×105=2.4×106 F=2.4μFC_{total} = \frac{1}{4.167 \times 10^5} = 2.4 \times 10^{-6} \text{ F} = 2.4 \mu\text{F}
  2. Calculate total charge stored using Q=CtotalVQ = C_{total}V: Qtotal=(2.4×106 F)×(12 V)=2.88×105 CQ_{total} = (2.4 \times 10^{-6} \text{ F}) \times (12 \text{ V}) = 2.88 \times 10^{-5} \text{ C} Therefore, total capacitance is 2.4μF2.4 \mu\text{F} and total charge is 28.8μC28.8 \mu\text{C}.

(b) In Parallel:

  1. Use the parallel capacitance formula: Ctotal=C1+C2C_{total} = C_1 + C_2 Ctotal=4.0μF+6.0μF=10.0μFC_{total} = 4.0 \mu\text{F} + 6.0 \mu\text{F} = 10.0 \mu\text{F}
  2. Calculate total charge stored using Q=CtotalVQ = C_{total}V: Qtotal=(10.0×106 F)×(12 V)=1.2×104 CQ_{total} = (10.0 \times 10^{-6} \text{ F}) \times (12 \text{ V}) = 1.2 \times 10^{-4} \text{ C} Therefore, total capacitance is 10.0μF10.0 \mu\text{F} and total charge is 120μC120 \mu\text{C}.

Worked example 2

A 2200 µF capacitor is charged by a 10.0 V power supply. It is then disconnected and connected in parallel with an uncharged 4700 µF capacitor. Calculate: (a) the initial energy stored in the 2200 µF capacitor. (b) the final potential difference across the combination. (c) the total energy stored in the combination after connection. (d) the energy lost during the connection.

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(a) Initial Energy Stored: Use the formula E=12CV2E = \frac{1}{2}CV^2. Einitial=12×(2200×106 F)×(10.0 V)2E_{initial} = \frac{1}{2} \times (2200 \times 10^{-6} \text{ F}) \times (10.0 \text{ V})^2 Einitial=0.11 JE_{initial} = 0.11 \text{ J}

(b) Final Potential Difference:

  1. First, find the initial charge stored on the first capacitor. This charge is conserved. Qinitial=C1V1=(2200×106 F)×(10.0 V)=0.022 CQ_{initial} = C_1 V_1 = (2200 \times 10^{-6} \text{ F}) \times (10.0 \text{ V}) = 0.022 \text{ C}
  2. When connected in parallel, this total charge is shared across the total capacitance. Ctotal=C1+C2=2200μF+4700μF=6900μFC_{total} = C_1 + C_2 = 2200 \mu\text{F} + 4700 \mu\text{F} = 6900 \mu\text{F}
  3. The new potential difference is found using V=Q/CV = Q/C. Vfinal=QtotalCtotal=0.022 C6900×106 F=3.188... V3.19 VV_{final} = \frac{Q_{total}}{C_{total}} = \frac{0.022 \text{ C}}{6900 \times 10^{-6} \text{ F}} = 3.188... \text{ V} \approx 3.19 \text{ V}

(c) Final Energy Stored: Use the total capacitance and final voltage. Efinal=12CtotalVfinal2E_{final} = \frac{1}{2} C_{total} V_{final}^2 Efinal=12×(6900×106 F)×(3.188... V)2E_{final} = \frac{1}{2} \times (6900 \times 10^{-6} \text{ F}) \times (3.188... \text{ V})^2 Efinal=0.0351... J0.035 JE_{final} = 0.0351... \text{ J} \approx 0.035 \text{ J}

(d) Energy Lost: The energy lost is the difference between the initial and final stored energy. Elost=EinitialEfinal=0.11 J0.0351 J=0.0749 J0.075 JE_{lost} = E_{initial} - E_{final} = 0.11 \text{ J} - 0.0351 \text{ J} = 0.0749 \text{ J} \approx 0.075 \text{ J} This energy is dissipated as heat in the connecting wires as the charge redistributes.