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Maxwell's Equations

Reading time: 12 minConfidence: HighLast verified: July 2026

Maxwell's equations are a set of four coupled partial differential equations that describe how electric and magnetic fields are generated and altered by electric charges, currents, and by each other, and together predict the existence of electromagnetic waves travelling at the speed of light.

Overview: the four equations (integral form)

#NameWhat it says
1Gauss's LawElectric charge produces a diverging electric field
2Gauss's Law for MagnetismThere are no magnetic monopoles — magnetic field lines always close on themselves
3Faraday's Law of InductionA changing magnetic field creates a circulating electric field
4Ampère-Maxwell LawElectric current and a changing electric field both create a circulating magnetic field
One sentence that captures itElectricity and magnetism are not two separate phenomena — they are two faces of a single electromagnetic field, each capable of generating the other, and light itself is that field propagating through empty space.

1. Gauss's Law

∇ · E = ρ/ε₀
SymbolNameSI Unit
EElectric fieldV/m
ρElectric charge densityC/m³
ε₀Vacuum permittivityF/m

Conditions of validity: Holds in vacuum and, with the substitution of the material's permittivity, inside dielectric media. Valid at all field strengths encountered in classical electromagnetism; at extremely high field strengths approaching the Schwinger limit, quantum electrodynamic corrections become relevant.

Derivation sketch (from Coulomb's law): Starting from Coulomb's law for a point charge, F = kq₁q₂/r², and defining the electric field as force per unit test charge, integrating the resulting field over any closed surface enclosing a charge distribution and applying the divergence theorem yields ∇·E = ρ/ε₀ directly — Gauss's law is mathematically equivalent to Coulomb's law, just expressed in differential rather than force form.

2. Gauss's Law for Magnetism

∇ · B = 0
SymbolNameSI Unit
BMagnetic fieldtesla (T)

Conditions of validity: Holds universally in all classical electromagnetism experiments performed to date. No isolated magnetic monopole (a particle with net "magnetic charge") has ever been observed, though some grand unified theories predict their existence at energy scales far beyond current experimental reach.

3. Faraday's Law of Induction

∇ × E = −∂B/∂t
SymbolNameSI Unit
EElectric fieldV/m
BMagnetic fieldtesla (T)
tTimeseconds (s)

Conditions of validity: Valid for all classical (non-quantum) electromagnetic phenomena. This is the physical principle behind every electric generator, transformer, and induction motor: a changing magnetic flux through a loop of wire induces an electromotive force around that loop.

Common mistakeFaraday's law is not merely "moving a magnet near a wire creates current" — it is the more general statement that any time-varying magnetic field, anywhere, creates a circulating electric field in space, whether or not a physical wire is present to carry the resulting current.

4. Ampère-Maxwell Law

∇ × B = μ₀J + μ₀ε₀(∂E/∂t)
SymbolNameSI Unit
BMagnetic fieldtesla (T)
JElectric current densityA/m²
μ₀Vacuum permeabilityN/A²
EElectric fieldV/m

Historical significance: The original Ampère's circuital law included only the current term (μ₀J). Maxwell's crucial 1861–1862 addition of the second term — the "displacement current," μ₀ε₀(∂E/∂t) — was necessary for mathematical self-consistency (charge conservation) and had the remarkable consequence of predicting self-sustaining electromagnetic waves, before any such wave had been observed experimentally.

Derivation of the electromagnetic wave equation

Taking the curl of Faraday's law, ∇ × (∇ × E) = −∂/∂t(∇ × B), and substituting the Ampère-Maxwell law (in vacuum, with J = 0) for ∇ × B, together with the vector identity ∇ × (∇ × E) = ∇(∇·E) − ∇²E and Gauss's law (∇·E = 0 in vacuum), yields:

∇²E = μ₀ε₀(∂²E/∂t²)

This is the standard wave equation, with wave speed v = 1/√(μ₀ε₀). Substituting CODATA values for μ₀ and ε₀ gives v ≈ 299,792,458 m/s — exactly the measured speed of light. This numerical coincidence, discovered by Maxwell in 1862, was the first evidence that light itself is an electromagnetic wave.

Worked example

Confirm the wave-speed prediction: using μ₀ = 1.25663706127 × 10⁻⁶ N/A² and ε₀ = 8.8541878188 × 10⁻¹² F/m (CODATA 2022), compute v = 1/√(μ₀ε₀).

μ₀ε₀ = 1.25663706127 × 10⁻⁶ × 8.8541878188 × 10⁻¹² ≈ 1.11265 × 10⁻¹⁷

v = 1/√(1.11265 × 10⁻¹⁷) ≈ 2.998 × 10⁸ m/s — matching c to within measurement precision, as expected since ε₀ is now defined self-consistently with the exact value of c.

Related equations

Primary Sources

  • Maxwell, J.C. (1865). "A Dynamical Theory of the Electromagnetic Field." Philosophical Transactions of the Royal Society of London, 155, 459–512.
  • Maxwell, J.C. (1873). A Treatise on Electricity and Magnetism. Oxford: Clarendon Press. Public domain.
  • Griffiths, D.J. (2017). Introduction to Electrodynamics, 4th ed. Cambridge University Press, Ch. 7.
  • Jackson, J.D. (1998). Classical Electrodynamics, 3rd ed. Wiley, Ch. 6.
Last verified: July 2026 · Source: Maxwell (1865, 1873); Griffiths (2017) · Confidence: high