Electromagnetic induction is the process by which a changing magnetic field within a closed conductor induces an electromotive force (EMF) and consequently an electric current in the conductor. Discovered by Michael Faraday in 1831, it is governed by Faraday's Law and Lenz's Law, and forms the operational basis of virtually all large-scale electrical power generation, transformers, and countless sensing devices. The phenomenon demonstrates the deep relationship between electricity and magnetism, first unified in Maxwell's equations.
EMF = −N(dΦ_B/dt) or EMF = Blv (for a conductor moving in a field)
LaTeX: \mathcal{E} = -N\frac{d\Phi_B}{dt} = Blv
| Symbol | Meaning | Unit |
|---|---|---|
| ℰ | Induced EMF | Volt (V) |
| N | Number of coil turns | Dimensionless |
| dΦ_B/dt | Rate of change of magnetic flux | Wb/s |
| B | Magnetic field strength | Tesla (T) |
| l | Length of conductor in the field | Metre (m) |
| v | Velocity of conductor | Metre per second (m/s) |
Problem
A straight conductor of length 0.5 m moves with a velocity of 4 m/s perpendicular to a uniform magnetic field of 0.8 T. Calculate the motional EMF induced in the conductor.
Solution
Step 1: Identify the formula for motional EMF. ℰ = Blv (conductor moving perpendicular to field) Step 2: Substitute the values. B = 0.8 T, l = 0.5 m, v = 4 m/s Step 3: Calculate. ℰ = 0.8 × 0.5 × 4 ℰ = 1.6 V
Answer
Induced motional EMF = 1.6 V
| Method | What Changes | Practical Device | Example Application |
|---|---|---|---|
| Moving a magnet near a coil | Magnetic flux through coil | Generator | Power station turbine |
| Moving a coil in a magnetic field | Flux linkage with coil | AC/DC Generator | Bicycle dynamo |
| Changing current in nearby coil | Flux from primary coil | Transformer | Power transmission |
| Rotating a coil in a field | Angle θ between B and A | Alternator | Car alternator |
| Moving a conductor across field lines | Flux through formed circuit | Motional EMF source | Rail gun, MHD drive |
PhET Faraday's Electromagnetic Lab
Full simulation of electromagnetic induction with magnets and coils
Open ToolKhan Academy — Electromagnetic Induction
Video series explaining electromagnetic induction from first principles
Open ToolBrilliant — Electromagnetic Induction
Interactive problems and detailed derivations on electromagnetic induction
Open ToolWikimedia Commons, CC BY-SA
Magnetic flux is the total quantity of magnetic field lines passing perpendicularly through a given surface area, measuring how much of the magnetic field is captured by that surface. It is a scalar quantity defined as the dot product of the magnetic field vector and the area vector of the surface. Magnetic flux is fundamental to understanding electromagnetic induction, transformer operation, and the behaviour of inductors in circuits.
Faraday's Law of Induction states that the electromotive force (EMF) induced in a closed loop is equal to the negative rate of change of magnetic flux through the loop. This fundamental law explains how changing magnetic fields produce electric currents, forming the basis of electric generators, transformers, and induction motors. It was discovered experimentally by Michael Faraday in 1831 and independently by Joseph Henry around the same time.
Lenz's Law states that the direction of an induced current is always such as to oppose the change in magnetic flux that caused it, thereby acting against the motion or change producing the induction. It is essentially a consequence of the conservation of energy and provides the negative sign in Faraday's Law of Induction. Named after Heinrich Lenz (1804–1865), the law explains why generators require mechanical work to produce electricity and underlies the principle of electromagnetic braking.
"Electromagnetic" combines "electric" (from Greek "elektron", meaning amber) and "magnetic" (from Greek "magnetes lithos", stone from Magnesia). "Induction" from Latin "inductio" meaning "a leading into". Faraday coined the concept of electromagnetic induction in 1831.