Physics › Magnetic fields › Transformers
Transformers
Two coils share a core, and Faraday's law does the rest: the turns ratio sets the voltage ratio. Real transformers lose a little power as heat in the windings and the core, and the national grid depends on one consequence, that transmitting at high voltage means small current and small losses in the cables.
Pick your board and the few notes written for the other boards quietly fold away, here and in the practice players. Nothing is deleted: every folded piece reopens on a tap.
Builds on Electromagnetic induction: Faraday and Lenz and Alternating currents.
IN THIS TOPIC
- Explain transformer operation through alternating flux and induced emf.
- Use the turns-ratio equation, and say why a transformer needs ac.
- Name the four causes of inefficiency, and use the efficiency equation.
- Calculate transmission-line power losses, and explain the high-voltage grid.
COMMON MISCONCEPTION
A transformer can step up power.
Where the power leaks
An ideal transformer passes power through untouched, and with the output power IsVs and input power IpVp, the report card is
Real transformers reach efficiencies in the high nineties of per cent, and the shortfall has nameable causes. The windings have resistance and warm up as current flows.
The changing flux induces eddy currents in the iron core itself, swirling charge that heats the metal; building the core from thin insulated laminations cuts those loops small and is the standard fix. A little flux leaks, missing the secondary, and a little energy is spent repeatedly re-magnetising the core each cycle. Whenever a question asks, name all four, since each carries its own mark. Stepping the voltage up steps the current down by at least the same factor, because the power out can never exceed the power in.
GUIDED PRACTICE
An efficiency from four meters
The charger above draws 0.52 A at 230 V and delivers 9.0 A at 12 V. Find its efficiency.
Show the working
Input is 230 × 0.52 = 120 W, and output is 12 × 9.0 = 108 W.
Efficiency = 108/120 = 0.90, or 90%. The missing tenth warms the windings and the core. Chargers run warm for that reason alone, and the four causes of loss above are worth naming by heart.
The grid's one big idea
Transmission cables have resistance, and the power they waste is P = I2R, so the current, squared, is what dominates the loss. For a fixed power delivered, P = IV, so raising the voltage lowers the current in proportion, and the squared dependence turns a modest voltage increase into a dramatic collapse in losses. Twenty-five times the voltage means six hundred and twenty-five times less power lost in the same cables. That is the logic of the national grid. Step up to hundreds of kilovolts at the power station, cross the country at small current, step back down near the user. Mains electricity is ac in the first place because transformers exist.
ASSESSMENT FOCUS
- The operation answer is a Faraday chain. Alternating primary current, alternating core flux, changing flux linkage in the secondary, induced emf. Four links, in that order.
- Transformers work on ac only, because induction needs changing flux. The dc case scores as a mark of its own, with steady flux and therefore no emf.
- The four inefficiency causes make a list question. Winding resistance, eddy currents that laminations reduce, flux leakage, and the energy of repeatedly magnetising the core.
- Grid questions want the argument in symbols. Fixed P = IV, so higher V means lower I, and the cable loss I2R falls as the square. Name that square explicitly.
- In efficiency calculations keep primary and secondary quantities strictly apart; the subscripts are where the marks hide.
- Both equations here are printed on the AQA data sheet, and neither comes with its caveat printed alongside. Supply it yourself. The turns ratio assumes every line of flux links both coils, and real cores leak a little, which is one reason a measured secondary voltage sits slightly low.
CHECK YOURSELF
A station sends 10 MW down cables of total resistance 5.0 Ω. Find the power lost when transmitting at 25 kV, and at 400 kV, as a percentage of the power sent each time.
Show a hint
Current first from P = IV; then the loss is that current squared times R.
Show the answer
At 25 kV the current is I = P/V = 107/(2.5 × 104) = 400 A, so the loss is I2R = 4002 × 5.0 = 8.0 × 105 W, or 0.80 MW, which is 8.0% of the power sent.
At 400 kV the current falls to 25 A, so the loss is 252 × 5.0 = 3.1 × 103 W, or 3.1 kW, a mere 0.031%.
Sixteen times the voltage, 256 times less loss. That is the square at work, and the reason pylons carry hundreds of kilovolts.
Turns set the voltage ratio; power only ever passes through.
The grid starves I²R with high volts, small current and tiny loss.
WORKBOOK
Printable practice for this topic: original exam-style questions with room to work, and a fully worked answer book. Free to use; please do not redistribute or sell.
Or read them with their mark schemes on the transformers questions page.
WHERE TO GO NEXT
- Rearranging equations is the maths this lesson leans on, worked through from GCSE.
CHECK YOUR PROGRESS
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- Explain transformer operation through alternating flux and induced emf.
- Use the turns-ratio equation, and say why a transformer needs ac.
- Name the four causes of inefficiency, and use the efficiency equation.
- Calculate transmission-line power losses, and explain the high-voltage grid.
Open the full revision checklist to track your progress across the whole unit.