EM Induction

EM Induction

Updated Mar 26, 2026

In 1831, Michael Faraday discovered something that quite literally changed the world: a changing magnetic field can create an electric current — without any battery or power source. Move a magnet through a coil of wire and a current flows. Stop moving the magnet and the current stops. Move it the other way and the current reverses.

This is electromagnetic induction, and it’s the principle behind every electrical generator, every transformer in every power line, every induction cooktop, every wireless phone charger, and every MRI machine. Your wall outlets exist because Faraday figured this out.

If you’ve studied electric fields and magnetic fields, you know that these fields can exert forces on charges. Induction goes a step further: a changing magnetic field can actually create an electric field, which then pushes charges around a circuit.

Magnetic Flux

Faraday's electromagnetic induction experiment showing a magnet being moved through a coil of wire, inducing an EMF and current in the coil
Faraday's induction experiment. Moving a magnet into or out of a coil changes the magnetic flux through the coil, inducing an EMF and driving a current. The faster the magnet moves, the larger the induced EMF. Credit: Wikimedia Commons, CC BY-SA

Before we can talk about induction, we need the concept of magnetic flux - the total amount of magnetic field passing through a surface.

Magnetic flux (Φ\Phi) through a surface is:

Φ=BAcosθ\displaystyle \Phi = BA \cos\theta

where BB = magnetic field (T), AA = area of the loop (m²), and θ\theta = angle between BB and the normal (perpendicular) to the surface. The unit of flux is the weber (Wb), where 1 Wb = 1 T·m².

Flux is maximum when the field is perpendicular to the surface (θ=0°\theta = 0°, cosθ=1\cos\theta = 1) and zero when the field is parallel to the surface (θ=90°\theta = 90°, cosθ=0\cos\theta = 0).

Faraday’s Law (Conceptual)

Faraday’s law states that a changing magnetic flux through a loop induces an EMF (voltage) in the loop. The faster the flux changes, the larger the induced EMF.

Three ways to change flux (and induce an EMF):

  1. Change BB - move a magnet closer to or farther from the loop, or turn an electromagnet on/off.
  2. Change AA - expand or contract the loop (like pulling a wire through a field).
  3. Change θ\theta - rotate the loop in the field (this is how generators work).

Lenz’s Law

Lenz’s law tells you the direction of the induced current: the induced current flows in a direction that opposes the change in flux that caused it.

Applying Lenz’s Law Step by Step

  1. Determine the direction of the external magnetic field through the loop.
  2. Determine whether the flux is increasing or decreasing.
  3. The induced current will create a magnetic field that opposes the change:
    • If flux is increasing, the induced field opposes the external field (points opposite).
    • If flux is decreasing, the induced field supports the external field (points same direction).
  4. Use the right-hand rule to find the current direction that produces the needed induced field.

Example

A bar magnet with its north pole pointing down is dropped toward a horizontal loop of wire. The downward magnetic flux through the loop is increasing. By Lenz’s law, the induced current must create an upward magnetic field to oppose the increase. Using the right-hand rule, this means the current flows counterclockwise when viewed from above.

Applications

Generators

A generator is the reverse of a motor. A motor takes current and produces rotation. A generator takes rotation and produces current. Spinning a wire loop in a magnetic field continuously changes the flux (by changing θ), inducing an alternating EMF. That’s the basis of AC power generation at every power plant.

Transformers

A transformer uses electromagnetic induction to change the voltage of AC power. Two coils (primary and secondary) are wound around a shared iron core. Alternating current in the primary coil creates a changing magnetic field, which induces an EMF in the secondary coil.

The voltage ratio depends on the number of turns:

V2V1=N2N1\displaystyle \dfrac{V_2}{V_1} = \dfrac{N_2}{N_1}

A step-up transformer (N2>N1N_2 > N_1) increases voltage. A step-down transformer (N2<N1N_2 < N_1) decreases voltage. Energy is conserved (ideally): if voltage goes up, current goes down proportionally.

Eddy Currents

When a conducting material (not just a wire loop) is exposed to a changing magnetic field, induced currents swirl through the bulk of the material. These are called eddy currents. They oppose the change in flux (Lenz’s law) and dissipate energy as heat. Eddy currents are why:

  • A metal pendulum swinging between the poles of a magnet slows down rapidly.
  • Induction cooktops heat metal pots without a flame.
  • Electromagnetic brakes work without friction pads.
A circular wire loop is in a region where the magnetic field is increasing. According to Lenz's law, in what direction does the induced current flow?
Click to reveal answer
The induced current flows in the direction that creates a magnetic field opposing the increase. If the external field points into the page and is increasing, the induced current must create a field pointing out of the page (to oppose the increase). By the right-hand rule, this means the current flows counterclockwise (when viewed from the side where the field is coming out).
A transformer has 100 turns in the primary coil and 500 turns in the secondary. If the input voltage is 120 V, what is the output voltage? Is this a step-up or step-down transformer?
Click to reveal answer
V2=V1(N2/N1)=120 V×(500/100)=600V_2 = V_1(N_2/N_1) = 120 \text{ V} \times (500/100) = 600 V. This is a step-up transformer (N2>N1N_2 > N_1, so voltage increases). By conservation of energy, the output current will be 15\frac{1}{5} of the input current (if the input current is 2 A, the output current is 0.4 A).