Physics

Faraday's Law & Induction

Visualize electromagnetic induction, magnetic flux, and the resulting electromotive force from a rotating coil.

Faraday's Law of Induction

Concept Overview

Faraday's Law of Induction is a fundamental principle in electromagnetism that describes how a changing magnetic field induces an electromotive force (EMF) in a closed circuit. This principle is the basis for how electric generators, transformers, and many other electrical machines operate. The magnitude of the induced EMF is directly proportional to the rate of change of magnetic flux through the circuit.

Mathematical Definition

Magnetic flux (ΦB) measures the total magnetic field passing through a given area. It depends on the magnetic field strength B, the loop area A, and the angle θ between the magnetic field vector and the area normal vector:

ΦB = B · A · cos(θ)

Faraday's Law states that the induced EMF (ε) in a closed loop equals the negative rate of change of magnetic flux. For a coil with N turns:

ε = −N · (dΦB / dt)

For a coil rotating with angular velocity ω (so θ = ωt), differentiating ΦB gives the peak EMF:

ε(t) = N · B · A · ω · sin(ωt)

Key Concepts

  • Magnetic Flux: A scalar measure of how much magnetic field passes through a surface, weighted by the cosine of the angle between B and the surface normal.
  • Lenz's Law: The negative sign in Faraday's Law encodes Lenz's Law — the induced current always flows in a direction that opposes the change in flux that produced it, acting as a brake on the change.
  • Motional EMF: When a conductor moves through a magnetic field, free charges experience a Lorentz force (F = qv × B) that separates them, creating a potential difference (EMF) across the conductor's ends.
  • Mutual Inductance: Two coils placed near each other share flux. A changing current in one coil induces an EMF in the other, the basis for transformers.
  • Self-Inductance (L): A single coil opposes changes in its own current. The back-EMF is ε = −L · (dI/dt), where L is the inductance in henries (H).

Historical Context

Michael Faraday discovered electromagnetic induction experimentally in 1831 while working at the Royal Institution in London. By moving a magnet in and out of a coil of wire, he observed a transient current — proving that a changing magnetic field could drive electricity. Independently, Joseph Henry made a similar discovery in the United States around the same time. James Clerk Maxwell later formalized Faraday's observations into a mathematical law, which became one of the four Maxwell's equations that unify classical electromagnetism.

Real-world Applications

  • Electric Generators: Rotate a coil in a magnetic field to continuously change flux and produce alternating current (AC) — the foundation of power plants worldwide.
  • Transformers: Use mutual induction between two coils to step AC voltage up or down for efficient long-distance power transmission.
  • Induction Motors: A rotating magnetic field in the stator induces currents in the rotor, generating torque without any physical contact.
  • Wireless Charging: A transmitter coil produces a time-varying magnetic field that induces an EMF in a receiver coil inside the device, enabling contactless power transfer.
  • Metal Detectors: Transmit an alternating magnetic field; nearby conductive objects experience induced eddy currents that disturb the field, signaling their presence.

Related Concepts

  • Coulomb's Law & Electric Force — the electrostatic counterpart of electromagnetic interaction
  • Electromagnetic Waves — Maxwell's equations combining Faraday's Law with Ampère's Law predict light as a wave
  • Electric Field Lines — visualizing how induced fields extend through space

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