Kirchhoff's laws and combining resistorsEdexcel International A Level Physics: Revision notes
Section 1
Charge conservation and Kirchhoff's first law
Charge cannot be created or destroyed, and it does not build up at a point in a circuit. So at any junction the total current entering equals the total current leaving. This is Kirchhoff's first law:
In a series circuit there are no junctions, so the current is the same everywhere. In a parallel circuit the current splits at a junction and the branch currents add up to the total:
Use 'charge is conserved' as the reason for current statements, and 'energy is conserved' as the reason for p.d. statements.
Section 2
Energy conservation and Kirchhoff's second law
Each coulomb of charge gains energy from the source and transfers it to components. Around any closed loop the energy gained per unit charge equals the energy transferred per unit charge. This is Kirchhoff's second law: in a closed loop, the sum of the e.m.f.s equals the sum of the potential differences, .
For a single supply of p.d. with components in series, . Components in parallel are connected across the same two points, so they have the same p.d.
Parallel branches do not share the supply p.d.: each has the full p.d. across it. It is the current that divides.
Section 3
Resistors in series
Start from the two conservation laws. The current is the same through each resistor (charge). The supply p.d. is shared: (energy). With :
So for resistors , and the total is always larger than the largest resistor.
Section 4
Resistors in parallel
The total current splits: (charge). Each resistor has the same p.d. (energy). Using :
The total resistance is always smaller than the smallest resistor, because adding a branch gives the charge carriers another route. For two resistors, .
After adding 1/R₁ + 1/R₂, remember to take the reciprocal. For 6.0 Ω and 3.0 Ω, 1/R = 0.50 Ω⁻¹ so R = 2.0 Ω, not 0.50 Ω.
Section 5
Worked example
A 12 V battery (negligible internal resistance) is connected to a 10 Ω resistor in series with a 30 Ω and 60 Ω resistor in parallel.
- Parallel pair: , so Ω
- Total: Ω; A
- p.d. across the 10 Ω: V, so across the pair: V
- Branch currents: A and A, which add to 0.40 A
Must Know
- Kirchhoff 1: current into a junction = current out (conservation of charge)
- Kirchhoff 2: sum of e.m.f.s = sum of p.d.s around a loop (conservation of energy)
- Series: same I, V shares, R = R₁ + R₂
- Parallel: same V, I shares, 1/R = 1/R₁ + 1/R₂
- Be able to derive both from the two conservation laws
That's the notes covered.
Carry on to the next subtopic.
Exam questions on Kirchhoff's laws and combining resistors
- A technician connects a 12 V battery of negligible internal resistance in series with a 4.0 Ω resistor and an 8.0 Ω resistor.Calculate the potential difference across each resistor and show that your values are consistent with conservation of energy.2 marks
- A 6.0 Ω resistor and a 3.0 Ω resistor are connected in parallel across a 9.0 V battery of negligible internal resistance.Calculate the current in each resistor and show that the total current is consistent with conservation of charge.2 marks
- A teacher wants to show that the equations for combining resistors can be derived from conservation laws. She considers two resistors, R₁ and R₂, connected to a supply of potential difference V. First they are connected in series, with total current I, and then in parallel, with total current I.Use conservation laws to derive the equation for the total resistance R of two resistors in series.3 marks
Written by the Exaim team, led by Shaun Daswani (Head of Upper Secondary, Improve ME Institute; MSc Financial Mathematics, Imperial College London; BSc, UCL) and Jason Daswani (operational lead, Improve ME Institute; LSE).