What is Faraday's law of induction?

Faraday's law of induction: ℰ = −dΦ/dt. Change the magnetism passing through a coil of wire and a voltage appears in it, with no battery at all. The faster the change and the more turns of wire, the bigger the voltage, and the current it drives always pushes back against the change.

Push a magnet into a coil and a voltage appears from nowhere; hold it still and it vanishes. Play with the 1831 discovery that lights the world, then find it in transformers, fans, guitar pickups, induction hobs and a magnet that floats down a copper pipe.

Faraday's law of inductionOpened 27 Sept 202612 min to playFree · no sign-up

In 60 seconds

  1. Change makes voltage

    A voltage appears in a coil whenever the magnetic flux through it changes: ℰ = −N dΦ/dt. Push a magnet in and the meter kicks; hold it still inside and the reading is zero. Faster motion and more turns give more volts.

  2. Lenz's law: it always pushes back

    The induced current flows so that its own magnetism opposes the change. A north pole pushed into a coil meets a north pole pushing back. That is why generating electricity takes work, and why induction never makes free energy.

  3. Transformers need AC

    Two coils share the changing flux in an iron core, so the voltages go as the turns: V₂ ÷ V₁ = N₂ ÷ N₁. A UPS lifts 12 V to 230 V this way. Feed a transformer steady DC and nothing comes out.

  4. Motors and generators are one machine

    A fan's squirrel cage is dragged round by currents the rotating field induces in it, always slipping a little behind. Spin a motor instead and it generates: electric cars brake by charging their batteries.

  5. Eddy currents and light

    A magnet drifts slowly down a copper pipe, braked by the currents it induces. Induction hobs heat pans the same way. And Maxwell showed that changing fields can chase each other through space as light.

Where you'll meet it

ℰ = −dΦ/dt

EMF = −(number of turns) × (rate of change of magnetic flux): the faster the flux through a coil changes, the bigger the voltage, and it always pushes against the change

The history

From a twitching compass needle to the generators that make almost all the world's electricity.

Read the full history
  1. 1820A current moves a compass
  2. 1831Magnets make electricity
  3. 1865Light is an electromagnetic wave
  4. 1885The practical transformer
  5. 1902Power from the Kaveri falls

The full explanation

Faraday's law of induction, chapter by chapter

Chapter 1

Change the flux, make a voltage

A magnet moving near a coil pushes current round it. Only change counts.

Wrap wire into a coil, join its ends to a meter, and push a magnet in. The needle kicks. Hold the magnet still and the needle falls back to zero, even with the magnet deep inside. Pull it out and the needle kicks the other way. Michael Faraday found this on 29 August 1831.

The magnet's field lines loop from its north pole round to its south. The amount of field passing through the coil is the magnetic flux, Φ, measured in webers (Wb). For a flat coil in an even field it is Φ = B × A × cos θ: field strength times area, times how squarely the coil faces the field.

Faraday's law: the voltage made in a coil equals how fast the flux through it changes, times the number of turns. ℰ = −N × dΦ/dt. Move faster and the same change happens in less time, so the voltage is bigger. Twice the turns, twice the voltage.

The minus sign is Lenz's law. The current always flows so that the coil's own magnetism fights the change. Push a north pole in and the coil's near end becomes a north pole that pushes back. Pull it away and that end turns south and tugs it back. That's why you must do work to make electricity: it isn't free.

Spin a coil in a steady field instead and its flux rises and falls smoothly, so it makes a sine wave of alternating voltage. That is a generator, and it is how almost all the world's electricity is made.

Try “The law, live” in the interactive model →

Chapter 2

Transformers and wireless chargers

A changing current in one coil makes a voltage in another, with nothing joining them.

Faraday's very first discovery was two coils wound on one iron ring. Switch a current on in one and a needle kicks on the other, though no wire joins them. A current makes flux; changing flux makes a voltage. That is mutual induction.

A transformer feeds the first coil, the primary, with AC. Its flux swings back and forth fifty times a second round an iron core, and passes through the secondary. Every turn of wire on the core feels the same volts, so the voltages go as the turns: V₂ ÷ V₁ = N₂ ÷ N₁. A phone-charger style transformer with 1,150 turns on the 230 V side and 60 on the other gives 12 V.

A home inverter (UPS) uses one backwards: its electronics chop the 12 V battery into AC and a 1 : 19 transformer lifts it to 230 V. A microwave oven steps 230 V up to about 2,000 V for its magnetron. See UPSClear and MicrowaveClear.

Why AC? Feed a transformer steady DC and the flux stops changing, so the secondary gets nothing. Worse, only the thin wire's resistance limits the primary's current, and it cooks. That's a big reason the world's grids run on AC.

A wireless phone charger is a transformer with the core taken out and a gap in the middle. Its flat coil runs at over 100,000 cycles a second. Lift the phone or slide it off-centre and less flux reaches the phone's coil, so charging slows and more power turns to heat.

Try “Two coils, no contact” in the interactive model →

Chapter 3

Motors are generators too

A fan’s rotor is pushed by currents it makes itself. An electric car brakes by making electricity.

An electric motor and a generator are the same machine. Push current in and it turns; turn it and current comes out. Induction is at work either way.

A desk or ceiling fan uses an induction motor. The coils round the outside, the stator, are fed AC in a pattern that makes a rotating magnetic field. In the middle sits a squirrel cage: aluminium or copper bars joined by rings, with no wires going in at all.

The rotating field sweeps past the bars, the flux through each loop of the cage changes, and Faraday's law drives current round the cage. Lenz's law says that current fights the change, so the cage gets dragged along after the field. It can never quite catch up: at the same speed the flux would stop changing and the push would vanish. The gap is the slip. See FanClear.

Other home machines use cousins of this. A mixer's universal motor has brushes and a wound rotor, and a modern washing machine uses a brushless DC motor driven by electronics. Spin any of them by hand and they make a voltage, the back-EMF, which rises with speed and holds the current down. See MixerClear and WasherClear.

An electric car uses this on purpose. Lift off the accelerator and the motor becomes a generator: the wheels spin it, it makes current that charges the battery, and Lenz's drag slows the car. That is regenerative braking. See CarClear.

Try “Motors and brakes” in the interactive model →

Chapter 4

Guitar pickups and induction hobs

A vibrating string makes a voltage. A fast-changing field heats a pan from the inside.

An electric guitar has no microphone. Under the strings sits a pickup: small magnets wrapped in a coil of thousands of turns of hair-thin wire. The magnets magnetise the steel strings just above them.

Pluck a string and it swings towards and away from the magnet hundreds of times a second. Each swing changes the flux through the coil a little, and Faraday's law turns that into a tiny voltage that copies the string's motion. The amplifier makes it loud. The voltage follows the string's speed, so a higher note of the same size gives more signal. Fit a nylon string and there is no signal at all. See GuitarClear.

An induction hob runs a flat coil at tens of thousands of cycles a second. The changing flux induces swirling eddy currents in the pan's base, and their I²R heating cooks the food. The glass top only warms up from the hot pan.

The pan matters. In magnetic iron and steel the currents crowd into a skin only about 0.2 mm thick, and iron resists current far more than aluminium, so they heat strongly. Aluminium conducts too well and isn't magnetic, so a basic hob barely heats it and usually refuses to start. Glass has no free electrons at all.

Induction gets about 85% of its energy into the pan. A gas flame loses much of its heat round the sides. See ChimneyClear.

Try “Pickups and pans” in the interactive model →

Chapter 5

Where induction gets strange

Magnets that float down pipes, transformers that can’t make energy, and light itself.

Drop a strong magnet down a copper pipe and it drifts down like a feather, though copper isn't magnetic. As the magnet falls, the flux through each ring of the pipe changes, so eddy currents swirl round the pipe above and below it. By Lenz's law they oppose the fall: the ring below pushes up, the ring above pulls up. The faster it falls, the harder they push, so it settles at a slow terminal speed. A plastic pipe has no free electrons, and the magnet just drops. Trains, roller coasters and gym bikes use this silent eddy-current braking.

Myth-buster: “A transformer that steps 12 V up to 230 V makes extra energy.” No! Voltage goes up, but current goes down by the same factor. Power in = power out, minus a few percent of heat in the copper and iron. Induction moves energy around. It never makes it.

Superconductors push this to the limit. With zero resistance, induced currents never die away, so a superconductor keeps the flux through it frozen. Lower one onto a magnet and it floats, locked in place: quantum levitation.

The biggest surprise came from James Clerk Maxwell in the 1860s. He wrote Faraday's law together with the other rules of electricity and found that a changing magnetic field makes an electric field, and a changing electric field makes a magnetic one. Each can keep the other going as a wave, travelling at c = 1 ÷ √(μ₀ε₀), the speed of light. Light, radio, Wi-Fi and X-rays are all induction chasing itself through space.

Try “Surprises and limits” in the interactive model →

Test yourself

Frequently asked

A magnet sits perfectly still inside a coil. What does the meter read?

Zero: the flux is not changing. Faraday’s law needs a change of flux. A still magnet gives a big flux but no change, so ℰ = 0.

You push the magnet in twice as fast. The voltage pulse is…

twice as tall and half as long. The same change of flux happens in half the time, so dΦ/dt and the voltage double. The area under the pulse stays the same.

You push a north pole into a coil. What does the coil’s near end become?

A north pole that pushes back. Lenz’s law: the induced current opposes the change. A north pole facing the incoming north pole resists it, so you must do work.

A transformer has 1,150 turns on its 230 V primary. How many secondary turns give 12 V?

About 60. V₂ ÷ V₁ = N₂ ÷ N₁, so N₂ = 1,150 × 12 ÷ 230 = 60.

You connect a transformer to steady DC. What comes out of the secondary?

Nothing, once the switch-on blip is over. Steady current makes steady flux. No change of flux, no induced voltage.

Why does a wireless charger work worse through a thick case?

Less of the pad’s flux reaches the phone’s coil, so coupling and efficiency fall. Flux spreads out with distance. Weaker coupling means less induced voltage and more wasted heat.

Why can a fan’s squirrel-cage rotor never turn exactly as fast as the rotating field?

At the same speed the flux through the cage would stop changing, so no current and no push. Induction needs changing flux. The rotor must slip behind the field for current to flow in its bars.

A 4-pole induction motor runs on 50 Hz. How fast does its field turn?

1,500 rpm. Field speed = 120 × f ÷ poles = 120 × 50 ÷ 4 = 1,500 rpm. The rotor turns a little slower.

What slows an electric car during regenerative braking?

The motor, working as a generator: the induced current’s magnetic drag opposes the turning. Lenz’s law: the current the wheels generate makes a force that opposes their motion, and the energy goes into the battery.

Why does an electric guitar pickup give no signal from a nylon string?

Nylon isn’t magnetic, so its motion doesn’t change the flux in the coil. The pickup senses a moving magnetised string. Nylon can’t be magnetised, so the flux never changes.

What actually heats the pan on an induction hob?

Eddy currents induced in the pan’s base. The changing field induces currents in the metal, and their resistance turns them into heat right inside the pan.

Why does a cast-iron pan work better than an aluminium one on a basic induction hob?

In magnetic iron the currents crowd into a thin skin with high resistance, so they heat far more. Heating goes as √(f μ ρ). Iron’s high μ and ρ give it tens of times aluminium’s heating for the same coil current.

Why does a magnet fall slowly through a copper pipe but not a plastic one?

The falling magnet induces eddy currents in the copper that oppose its motion. Copper conducts, so the changing flux drives currents round the pipe. By Lenz’s law they brake the magnet. Plastic can’t carry currents.

A transformer steps 12 V up to 240 V. What happens to the current?

It falls to about a twentieth, so power stays about the same. Power in ≈ power out. Twenty times the voltage means about a twentieth of the current, less a little lost as heat.

What did Maxwell find by combining Faraday’s law with the other laws of electricity?

That changing electric and magnetic fields can travel as a wave at the speed of light. The equations allowed waves moving at 1 ÷ √(μ₀ε₀), which matched the measured speed of light.

Words worth knowing

Magnetic flux
How much magnetic field passes through an area, in webers (Wb); for a flat coil Φ = B × A × cos θ.
Electromagnetic induction
Making a voltage in a conductor by changing the magnetic flux through it.
EMF
Electromotive force: the voltage induced in a coil, even with no battery.
Lenz's law
The induced current always flows so as to oppose the change that caused it.
Transformer
Two coils on an iron core that change an AC voltage in the ratio of their turns.
Generator
A machine that turns motion into electricity by spinning coils and magnets past each other.
Eddy currents
Swirling currents induced inside solid metal by a changing field; they heat it and brake motion.
Slip
How far an induction motor's rotor lags behind its rotating field.

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