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Series and parallel circuits and Kirchhoff's laws (QCE Physics Unit 1)

Syllabus dot point

“Analyse series and parallel resistor combinations using Kirchhoff's current and voltage laws, including problems with mixed series and parallel branches”

9 min read

Quick answer

Series resistors share the same current and add directly (Rs=R1+R2+⋯R_s = R_1 + R_2 + \cdots), parallel resistors share the same voltage and combine reciprocally (1/Rp=1/R1+1/R2+⋯1/R_p = 1/R_1 + 1/R_2 + \cdots), and Kirchhoff's current law (junction rule) and voltage law (loop rule) let you solve any DC network by working from the equivalent resistance back to the individual branches.

Jump to a section
  1. What this dot point is asking
  2. Kirchhoff's current law (KCL)
  3. Kirchhoff's voltage law (KVL)
  4. Series circuits
  5. Parallel circuits
  6. Mixed circuits
  7. Examples in context
  8. Try this
  9. Exam-style questions

What this dot point is asking

QCAA wants you to analyse DC circuits made of resistors in series and parallel combinations. Two foundational laws apply: Kirchhoff's current law (charge conservation at junctions) and Kirchhoff's voltage law (energy conservation around loops). These let you derive every other circuit relationship.

Kirchhoff's current law (KCL)

The sum of currents into a junction equals the sum of currents out:

∑Iin=∑Iout\sum I_{\text{in}} = \sum I_{\text{out}}

This is conservation of charge. Charge does not pile up at a node.

Kirchhoff's voltage law (KVL)

The sum of potential differences around any closed loop is zero:

∑Vloop=0\sum V_{\text{loop}} = 0

This is conservation of energy. The total energy gained from sources equals the total energy dissipated in resistors around the loop.

Series circuits

Resistors are in series when they form a single line; the same current flows through each.

  • Equivalent resistance: Rseries=R1+R2+R3+⋯R_{\text{series}} = R_1 + R_2 + R_3 + \cdots
  • Same current through every resistor: I1=I2=I3=⋯I_1 = I_2 = I_3 = \cdots
  • Voltage divides in proportion to resistance: Vi=IRiV_i = I R_i.
  • Total voltage: Vtotal=V1+V2+V3+⋯V_{\text{total}} = V_1 + V_2 + V_3 + \cdots (by KVL).

A single break in a series circuit (one bulb out) stops current in the whole circuit; this is why old Christmas-tree lights wired in series all went dark when one bulb blew.

Parallel circuits

Resistors are in parallel when they share two common nodes; the same voltage is across each.

  • Equivalent resistance: 1Rparallel=1R1+1R2+1R3+⋯\frac{1}{R_{\text{parallel}}} = \frac{1}{R_1} + \frac{1}{R_2} + \frac{1}{R_3} + \cdots
  • Same voltage across every branch: V1=V2=V3=⋯V_1 = V_2 = V_3 = \cdots
  • Current divides in inverse proportion to resistance: Ii=V/RiI_i = V / R_i.
  • Total current: Itotal=I1+I2+I3+⋯I_{\text{total}} = I_1 + I_2 + I_3 + \cdots (by KCL).

The parallel resistance is less than the smallest of the individual resistances. Adding more parallel paths drops the equivalent resistance and increases the total current at fixed voltage.

For two parallel resistors specifically, Rp=R1R2/(R1+R2)R_p = R_1 R_2 / (R_1 + R_2) (the product over the sum).

Mixed circuits

Most real circuits combine series and parallel sections. Reduce them step by step:

  1. Identify a parallel block and replace with RpR_p.
  2. Combine series resistors into RsR_s.
  3. Repeat until one equivalent resistance remains.
  4. Use V=IRV = IR on the equivalent to get total current.
  5. Work backward, applying Vi=IRiV_i = I R_i for series sections and Ii=V/RiI_i = V / R_i for parallel branches.
Worked example

Three identical 6 Ω6\ \Omega resistors are connected to a 1212 V battery in parallel. We find the equivalent resistance, the total current, and the current through each branch.

Step 1: Find the parallel equivalent resistance

In a parallel circuit, we add the reciprocals of the individual resistances. Because all three resistors are identical, each contributes 16\tfrac{1}{6} to the sum.

1Rp=16+16+16=36=12,Rp=2.0 Ω\frac{1}{R_p} = \frac{1}{6} + \frac{1}{6} + \frac{1}{6} = \frac{3}{6} = \frac{1}{2}, \qquad R_p = 2.0\ \Omega

Note that the parallel equivalent is less than any single resistor, as expected.

Step 2: Find the total current from the battery

With the three parallel branches replaced by their equivalent Rp=2.0 ΩR_p = 2.0\ \Omega, Ohm's law gives the total current drawn from the supply.

Itotal=VRp=122.0=6.0 AI_{\text{total}} = \frac{V}{R_p} = \frac{12}{2.0} = 6.0\ \text{A}

Step 3: Find the current through each branch and apply KCL

Each parallel branch has the full supply voltage 1212 V across it, so each branch current follows from Ohm's law individually.

Ii=VRi=126=2.0 AI_i = \frac{V}{R_i} = \frac{12}{6} = 2.0\ \text{A}

Final answer: Rp=2.0 ΩR_p = 2.0\ \Omega, total current 6.06.0 A, and each branch carries 2.02.0 A. Kirchhoff's current law is satisfied: 3×2.0=6.03 \times 2.0 = 6.0 A.

Common traps
Adding parallel resistors directly
1/R1/R values add, not RR values. Two 6 Ω6\,\Omega resistors in parallel give 3 Ω3\,\Omega, not 12 Ω12\,\Omega.
Forgetting that parallel branches have the same voltage
This is the most useful single fact: at any parallel node, VV is common.
Treating a junction as having different currents on the same wire
Within a single segment between junctions, the current is the same at every point.
Applying KVL with the wrong signs
Going around a loop, voltage drops across resistors in the direction of current flow are negative; battery EMFs going from negative to positive terminal are positive. Pick a direction and stick with it.

Examples in context

Example 1. A Cairns suburban distribution board feeds six 40 W40 \text{ W} LED downlights wired in parallel across 240 V240 \text{ V}. Each draws I=P/V=0.167 AI = P/V = 0.167 \text{ A} for a total current of 1.0 A1.0 \text{ A} via Kirchhoff's junction rule, satisfying the 10 A10 \text{ A} lighting circuit breaker. If one lamp fails open-circuit, the other five remain on (parallel branches independent). Wiring the same six lamps in series would push each lamp to one-sixth of 240 V240 \text{ V} (40 V40 \text{ V}), well under rating, and any single failure would dark the whole bank, which is why residential lighting in Queensland is universally parallel.

Example 2. A Bremer River bridge 24 V24 \text{ V} navigation light is fed via a 35 m35 \text{ m} submarine cable whose total resistance is 1.2 ohms1.2 \text{ ohms}. The cable resistance and lamp (R=12 ohmsR = 12 \text{ ohms}) are in series, so I=24/(12+1.2)=1.82 AI = 24/(12+1.2) = 1.82 \text{ A}, with Vcable=IRcable=2.18 VV_{cable} = IR_{cable} = 2.18 \text{ V} dropped before the lamp. Engineers either upsize the cable or compensate with a higher source voltage to deliver the rated 24 V24 \text{ V} at the lamp terminals, a worked Kirchhoff's-voltage-law calculation common in QCAA EA Unit 1 stems.

Try this

Q1. State Kirchhoff's current law and voltage law. [2 marks]

  • Cue. ∑Iin=∑Iout\sum I_{in} = \sum I_{out} at a junction; ∑V=0\sum V = 0 around a loop.

Q2. Three resistors of 6.06.0, 3.03.0 and 2.0 ohms2.0 \text{ ohms} are connected in parallel across a 12 V12 \text{ V} supply. Calculate ReqR_{eq}, the total current, and the current in the 3.0 ohm3.0 \text{ ohm} branch. [4 marks]

  • Cue. 1/Req=1/6+1/3+1/2=11/R_{eq} = 1/6 + 1/3 + 1/2 = 1, so Req=1.0 ohmsR_{eq} = 1.0 \text{ ohms}; Itot=12 AI_{tot} = 12 \text{ A}; I3=4 AI_{3} = 4 \text{ A}.

Q3. A circuit has a 12 V12 \text{ V} EMF with 4.0 ohms4.0 \text{ ohms} in series with a parallel pair 6.0 ohms6.0 \text{ ohms} and 3.0 ohms3.0 \text{ ohms}. (a) Determine the equivalent resistance. (b) Calculate the current from the EMF and the voltage across the parallel pair. (c) Verify Kirchhoff's voltage law around one loop. [3+3+2 marks; ISMG: Analysis and interpretation]

  • Cue. (a) Req=4+2=6.0 ohmsR_{eq} = 4 + 2 = 6.0 \text{ ohms}; (b) I=2.0 AI = 2.0 \text{ A}, Vpar=4.0 VV_{par} = 4.0 \text{ V}; (c) 12−8−4=012 - 8 - 4 = 0.

Exam-style questions

Questions in the style of QCAA exam questions on this dot point, each with a worked answer. They are written by ExamExplained unless tagged "Past paper"; the year shows the paper a question is modelled on.

Year 11 SAC-style5 marks
Three resistors R1=4.0 ΩR_1 = 4.0\,\Omega, R2=6.0 ΩR_2 = 6.0\,\Omega and R3=12 ΩR_3 = 12\,\Omega are connected in a circuit with a 1212 V battery, where R2R_2 and R3R_3 are in parallel with each other, and that combination is in series with R1R_1. Find (a) the equivalent resistance, (b) the total current, and (c) the voltage across R2R_2.
Show worked answer →

(a) Equivalent resistance.

Parallel: 1/Rp=1/6+1/12=2/12+1/12=3/121/R_p = 1/6 + 1/12 = 2/12 + 1/12 = 3/12, so Rp=4.0 ΩR_p = 4.0\,\Omega.

Series total: Req=R1+Rp=4.0+4.0=8.0 ΩR_{\text{eq}} = R_1 + R_p = 4.0 + 4.0 = 8.0\,\Omega.

(b) Total current. Itotal=V/Req=12/8.0=1.5I_{\text{total}} = V / R_{\text{eq}} = 12 / 8.0 = 1.5 A.

(c) Voltage across R2R_2. Voltage across R1R_1: V1=IR1=(1.5)(4.0)=6.0V_1 = I R_1 = (1.5)(4.0) = 6.0 V.

Voltage across the parallel combination = 12−6=6.012 - 6 = 6.0 V. Since R2R_2 is in parallel, V2=6.0V_2 = 6.0 V.

Markers reward correct identification of the topology, parallel-combination formula, and use of Kirchhoff's voltage law to find V2V_2.

Practise this

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