Skip to main content
EnglandElectronicsSyllabus dot point

How does Thevenin's theorem reduce a complicated network to a single source and resistance, and when is power transfer greatest?

Thevenin's theorem: replacing a linear network by an equivalent electromotive force and series resistance, finding the Thevenin voltage and resistance, and the maximum power transfer condition.

An Eduqas A-Level Electronics answer on Thevenin's theorem: how to replace any linear two-terminal network by a single equivalent electromotive force in series with a resistance, how to find the Thevenin voltage and Thevenin resistance, and the maximum power transfer theorem with its impedance-matching consequence.

Generated by Claude Opus 4.813 min answer

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

Have a quick question? Jump to the Q&A page

Jump to a section
  1. What this dot point is asking
  2. The answer
  3. Examples in context
  4. Try this

What this dot point is asking

Eduqas wants you to apply Thevenin's theorem to replace a linear two-terminal network by a single electromotive force in series with a resistance, find the Thevenin voltage and Thevenin resistance, and state and use the maximum power transfer theorem. These tools turn a messy network into one a single load can be analysed against.

The answer

Thevenin's theorem

Finding the Thevenin voltage and resistance

Maximum power transfer

Examples in context

Thevenin's theorem is how engineers model a sensor's output stage, an amplifier's output, or a power supply rail as "a voltage behind a resistance", so the effect of any load is a one-line calculation. Maximum power transfer governs audio output matching and radio-frequency aerial design, where the aim is to push the most signal power into the load. By contrast, a mains power supply is built with a very low output (Thevenin) resistance so its output voltage barely sags under load, the opposite design goal.

Try this

Q1. State how you find the Thevenin resistance of a network. [2 marks]

  • Cue. Remove the load, replace voltage sources by shorts and current sources by opens, then find the resistance looking into the terminals.

Q2. A source has VTh=10 VV_\text{Th} = 10\ \text{V} and RTh=5.0 ΩR_\text{Th} = 5.0\ \Omega. Find the matched load resistance. [1 mark]

  • Cue. RL=RTh=5.0 ΩR_L = R_\text{Th} = 5.0\ \Omega.

Q3. For the source in Q2, find the maximum power delivered to a matched load. [2 marks]

  • Cue. Pmax=VTh24RTh=10020=5.0 WP_\text{max} = \frac{V_\text{Th}^2}{4 R_\text{Th}} = \frac{100}{20} = 5.0\ \text{W}.

Exam-style practice questions

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

Eduqas 20216 marksA potential divider has a 6.0 kΩ6.0\ \text{k}\Omega and a 3.0 kΩ3.0\ \text{k}\Omega resistor in series across a 9.0 V9.0\ \text{V} supply, with the output taken across the 3.0 kΩ3.0\ \text{k}\Omega resistor. Find the Thevenin equivalent (the Thevenin voltage and Thevenin resistance) seen at the output terminals.
Show worked answer →

Thevenin voltage (up to 3 marks): this is the open-circuit output, the unloaded divider value: VTh=9.0×3.06.0+3.0=9.0×13=3.0 VV_\text{Th} = 9.0 \times \dfrac{3.0}{6.0 + 3.0} = 9.0 \times \dfrac{1}{3} = 3.0\ \text{V}.

Thevenin resistance (up to 3 marks): replace the supply by a short circuit, leaving the two resistors in parallel as seen from the output terminals: RTh=6.0×3.06.0+3.0=189=2.0 kΩR_\text{Th} = \dfrac{6.0 \times 3.0}{6.0 + 3.0} = \dfrac{18}{9} = 2.0\ \text{k}\Omega.

Markers reward VTh=3.0 VV_\text{Th} = 3.0\ \text{V} (open-circuit voltage), shorting the source to find RThR_\text{Th}, and the parallel combination RTh=2.0 kΩR_\text{Th} = 2.0\ \text{k}\Omega.

Eduqas 20204 marksState the maximum power transfer theorem, and calculate the load resistance and the power delivered to it when a source of Thevenin voltage 12 V12\ \text{V} and Thevenin resistance 8.0 Ω8.0\ \Omega is matched.
Show worked answer →

Theorem (up to 1 mark): maximum power is transferred to the load when the load resistance equals the source (Thevenin) resistance, RL=RThR_L = R_\text{Th}.

Matched load (up to 1 mark): RL=RTh=8.0 ΩR_L = R_\text{Th} = 8.0\ \Omega.

Power delivered (up to 2 marks): at match the source voltage splits equally, so the load voltage is 6.0 V6.0\ \text{V} and P=VL2RL=6.028.0=368.0=4.5 WP = \dfrac{V_L^2}{R_L} = \dfrac{6.0^2}{8.0} = \dfrac{36}{8.0} = 4.5\ \text{W} (equivalently Pmax=VTh24RTh=14432=4.5 WP_\text{max} = \frac{V_\text{Th}^2}{4 R_\text{Th}} = \frac{144}{32} = 4.5\ \text{W}).

Markers reward the matching condition RL=RThR_L = R_\text{Th}, the value 8.0 Ω8.0\ \Omega, and the maximum power 4.5 W4.5\ \text{W}.

Related dot points

Sources & how we know this