law

Faraday's law of electromagnetic induction

Faraday's law of induction states that a changing magnetic field induces an electromotive force in a circuit.
54 related articles · 2 formulas · 2 who worked here

Description

Michael Faraday in 1831 long sought a connection between magnetism and electricity. His ingenious experiment with two windings on one iron ring showed: when current was switched on in the first coil, a momentary surge appeared in the second. He described it as 'converting magnetism into electricity.' Later, James Clerk Maxwell put the law into rigorous mathematical form. The essence: any change in a magnetic field over time generates a vortex electric field, even in a vacuum.

History

In the 1820s, Hans Christian Ørsted discovered that an electric current creates a magnetic field. Michael Faraday took on the reverse problem and after years of experiments, in 1831 observed a momentary current in the secondary winding when the primary circuit was closed. The results were reported to the Royal Society. Independently, Joseph Henry in the USA discovered the phenomenon in the same year but published later. James Clerk Maxwell included the law in his system of equations (1861–1862), adding the displacement current term for symmetry.

How it works

The operating principle of generators, transformers, magnetic sensors, hard disk recording. Limits of applicability: works in classical electrodynamics up to relativistic speeds, but at the quantum limit, accounting for fluctuations and charge discreteness requires a more detailed description.

In practice

Electric generators at all power plants, transformers, induction cooktops, and wireless chargers operate on this principle — converting motion into electricity.

Fun fact

If you drop a strong magnet into a copper pipe, it falls surprisingly slowly — induced currents (eddy currents) according to Lenz's law slow it down, as if an invisible hand is holding it.

Concept graph →

Formulas

$$\text{RM} = \frac{e^3}{2\pi m_e^2 c^4} \int n_e B_\parallel \, dl$$
Rotation measure is proportional to the integral of electron density times parallel magnetic field along the line of sight.
What is in the formula
n_evariableelectron number density — electron number density per cubic metre
B_parallelvariablemagnetic field component along line of sight — magnetic flux density tesla
dlvariableinfinitesimal path element along line of sight metre
econstantelementary charge — elementary charge = 1.602176634e-19 coulomb
m_econstantelectron rest mass — electron mass = 9.1093837015e-31 kilogram
cconstantspeed of light in vacuum — speed of light = 299792458 metre per second
∫operatorsummation over the line of sight — integral operator
{rm}=0.81\intn_eb_\paralleldl · 2606.22354
$$\frac{\partial \mathbf{B}}{\partial t} = \nabla \times (\mathbf{u} \times \mathbf{B}) + \eta \nabla^2 \mathbf{B}$$
Magnetic field evolution from flow advection and Ohmic diffusion.
What is in the formula
\mathbf{B}variableMagnetic field vector — magnetic field tesla
tvariableTime — time second
\mathbf{u}variableVelocity field of the conducting fluid — velocity metre per second
\etavariableMagnetic diffusivity — magnetic diffusivity square metre per second
\frac{\partial}{\paroperatorPartial derivative with respect to time — partial derivative
\nabla \timesoperatorCurl operator — curl operator
\nabla^2operatorLaplacian operator — laplacian operator
\frac{\partial{b}}{\partialt}=\nabla*({u}*{b})+\eta\nabla^2{b} · 2607.27531v1

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