Capacitors: Diagram-Based Questions (4)

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Question

In a circuit, three capacitors of 2μF2 \mu\text{F}, 3μF3 \mu\text{F}, and 6μF6 \mu\text{F} are connected: the 2μF2 \mu\text{F} and 3μF3 \mu\text{F} are in parallel, and that combination is in series with the 6μF6 \mu\text{F}, all connected across a 30 V30 \text{ V} battery. Find the equivalent capacitance, the charge on each capacitor, and the voltage across each.

Solution — Step by Step

For capacitors in parallel, capacitances add:

Cp=2+3=5μFC_p = 2 + 3 = 5 \mu\text{F}

For capacitors in series, reciprocals add:

1Ceq=15+16=6+530=1130\frac{1}{C_{\text{eq}}} = \frac{1}{5} + \frac{1}{6} = \frac{6 + 5}{30} = \frac{11}{30}

Ceq=30112.73μFC_{\text{eq}} = \frac{30}{11} \approx 2.73 \mu\text{F}

Qtotal=CeqV=3011×30=9001181.8μCQ_{\text{total}} = C_{\text{eq}} \cdot V = \frac{30}{11} \times 30 = \frac{900}{11} \approx 81.8 \mu\text{C}

In a series combination, this same charge flows onto the 6μF6 \mu\text{F} capacitor and onto the parallel block.

Voltage on 6μF6 \mu\text{F}:

V6=QC=900/116=1501113.6 VV_6 = \frac{Q}{C} = \frac{900/11}{6} = \frac{150}{11} \approx 13.6 \text{ V}

Voltage on the parallel block:

Vp=3013.6=16.4 V(or 900/115=180/11)V_p = 30 - 13.6 = 16.4 \text{ V} \quad \text{(or } \frac{900/11}{5} = 180/11)

The parallel branches share this voltage:

Q2=2×16.432.7μC,Q3=3×16.449.1μCQ_2 = 2 \times 16.4 \approx 32.7 \mu\text{C}, \quad Q_3 = 3 \times 16.4 \approx 49.1 \mu\text{C}

Check: Q2+Q3=81.8μCQ_2 + Q_3 = 81.8 \mu\text{C}. ✓

Why This Works

Capacitor combination rules are the opposite of resistor rules:

  • Series capacitors: 1/Ceq=1/Ci1/C_{\text{eq}} = \sum 1/C_i (like resistors in parallel)
  • Parallel capacitors: Ceq=CiC_{\text{eq}} = \sum C_i (like resistors in series)

The reason: in series, the same charge sits on each capacitor (charge can’t disappear at the junctions), so voltages add. In parallel, the same voltage appears across each, so charges add.

Alternative Method

Use energy: total energy stored is 12CeqV2=12×(30/11)×9001227μJ\tfrac{1}{2}C_{\text{eq}}V^2 = \tfrac{1}{2} \times (30/11) \times 900 \approx 1227 \mu\text{J}. Then verify by summing individual energies: 12×2×16.42+12×3×16.42+12×6×13.62\tfrac{1}{2} \times 2 \times 16.4^2 + \tfrac{1}{2} \times 3 \times 16.4^2 + \tfrac{1}{2} \times 6 \times 13.6^2. Useful as a sanity check on long capacitor problems.

In series capacitors, the smallest capacitor gets the highest voltage (it dominates). In parallel capacitors, the largest one gets the most charge. Use this as a quick MCQ check before your final answer.

Common Mistake

Students mix up series/parallel rules between capacitors and resistors. Memory aid: “capacitors store charge — in series, that one charge has to squeeze through everyone, so the smallest dominates.” That’s why the formula has reciprocals.

The other slip: assuming all capacitors carry the same charge in a parallel branch. They don’t — they carry the same voltage. Charges divide in proportion to capacitance: Qi=CiVpQ_i = C_i V_p.

Final answer: Ceq2.73μFC_{\text{eq}} \approx 2.73 \mu\text{F}, Q681.8μCQ_6 \approx 81.8 \mu\text{C}, V613.6 VV_6 \approx 13.6 \text{ V}, Vp16.4 VV_p \approx 16.4 \text{ V}, Q232.7μCQ_2 \approx 32.7 \mu\text{C}, Q349.1μCQ_3 \approx 49.1 \mu\text{C}.

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