Electromagnetismundergraduategraduate

Maxwell's Equations (Unified)

Also known as: Maxwell's Equations · Classical Electrodynamics

Two of the four equations say charges make diverging E-fields and that there are no magnetic charges; the other two say a changing B makes a curling E and a changing E (or a current) makes a curling B. That mutual feedback lets the fields regenerate each other and sail off as light — no charges required.

 ⁣ ⁣E=ρε0,  ⁣ ⁣B=0,  ⁣× ⁣E=tB,  ⁣× ⁣B=μ0J+μ0ε0tE\nabla\!\cdot\!\vec{E}=\tfrac{\rho}{\varepsilon_0},\ \nabla\!\cdot\!\vec{B}=0,\ \nabla\!\times\!\vec{E}=-\partial_t\vec{B},\ \nabla\!\times\!\vec{B}=\mu_0\vec{J}+\mu_0\varepsilon_0\partial_t\vec{E}
Live simulation
warming up the physics…

A traveling electromagnetic wave: the red E-field and blue B-field oscillate in perpendicular planes and march to the right; sliders set amplitude and frequency.

Equivalent forms

c=1μ0ε0c = \frac{1}{\sqrt{\mu_0\varepsilon_0}}
Aμ=μ0Jμ\Box A^\mu = \mu_0 J^\mu
μFμν=μ0Jν\partial_\mu F^{\mu\nu} = \mu_0 J^\nu
The same constants you measure with a capacitor and a coil fix the speed of light — electricity and magnetism were never separate, and neither is light.