Technopedia

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Electromagnetism

Electromagnetism is the branch of physics that describes electric and magnetic fields, the forces they exert on charges, and the propagation of light and radio waves. It is relevant whenever electric charge is present, current flows, magnetic materials respond, energy is transmitted by wires or radiation, or electromagnetic waves interact with matter.

Authoritative sources

Brief history

Categorization

The five classes separate the subject by field regime and first-principle role: static electric fields, static magnetic fields, near-field time-varying coupling, far-field radiation, and material response. Induction and radiation are not separate fundamental classes; they are near-field and far-field limits of the same time-varying Maxwell coupling.

PageRegimeGoverning law(s)Typical applicationRelation to other classes
ElectrostaticsCharges at restGauss's law ∇ ⋅ E⃗ = ρ/ε0, ∇ × E⃗ = 0Capacitors, shielding, electrostatic precipitatorsStatic limit of electrodynamics when time derivatives vanish
MagnetostaticsSteady currentsAmpère's law ∇ × B⃗ = μ0 J⃗, ∇ ⋅ B⃗ = 0Permanent magnets, inductors, MRI magnetsStatic limit of electrodynamics; magnetic fields have no monopole sources
ElectrodynamicsTime-varying fieldsFull Maxwell's equations, Faraday's law, Poynting theoremTransformers, induction heating, antennas (near field)Contains induction and quasi-static circuit theory; reduces to electrostatics and magnetostatics for slow fields
Electromagnetic RadiationPropagating wavesWave equation, dispersion, quantum: E = hνOptics, radio, X-rays, lasers, photodetectorsFar-field/high-frequency limit of electrodynamics; interacts with media
Electromagnetic MediaConstitutive response (applies to all regimes above)D⃗ = ε E⃗, B⃗ = μ H⃗, J⃗ = σ E⃗Dielectrics, superconductors, metamaterials, waveguidesModifies all field classes; sets wave speed, reflection, transmission, and loss

Lumped-element circuit theory (Kirchhoff laws, impedance, RC/RL/RLC, circuit power) is not a separate first-principle class. It is the quasi-static limit of electrodynamics, valid when circuit dimensions are much smaller than the wavelength, and should be read under the Electrodynamics class.

Details

The central force law is the Lorentz force: F=qE+qv×B\mathbf{F}=q\mathbf{E}+q\mathbf{v}\times\mathbf{B}. In vacuum, the fields obey Maxwell equations:

∇⋅E=ρε0,∇⋅B=0,∇×E=−∂B∂t,∇×B=μ0J+μ0ε0∂E∂t\nabla\cdot\mathbf{E}=\frac{\rho}{\varepsilon_0},\quad \nabla\cdot\mathbf{B}=0, \nabla\times\mathbf{E}=-\frac{\partial\mathbf{B}}{\partial t},\quad \nabla\times\mathbf{B}=\mu_0\mathbf{J}+\mu_0\varepsilon_0\frac{\partial\mathbf{E}}{\partial t}

Electrostatics and magnetostatics are the limits in which the time-derivative terms are negligible. Electrodynamics keeps those terms: Faraday law makes changing magnetic flux produce electric fields, and the Maxwell-Ampere term makes changing electric fields produce magnetic fields. Radiation is the far-field solution of the same coupled equations, while media replace vacuum constants with material response functions.