← Iris

Polarization Linear
Wavelength 1.0
Filter angle Off
Maxwell’s Equations
∇·E = ρ/ε₀
∇·B = 0
∇×E = −∂B/∂t
∇×B = μ₀J + μ₀ε₀∂E/∂t
Polarization:
Show:
Wavelength 1.0
Amplitude 1.0
Camera Angle 30°
Filter Angle
Phase Diff (Elliptical) 45°
Speed 1.0

Electromagnetic waves

James Clerk Maxwell showed in 1865 that changing electric fields create magnetic fields and vice versa. The result is a self-sustaining wave that propagates at the speed of light: c = 1/√(μ₀ε₀). Light, radio, X-rays, and gamma rays are all electromagnetic waves — differing only in wavelength.

Perpendicularity

The electric field E and magnetic field B are always perpendicular to each other and to the direction of propagation. In this visualization, the wave travels along the z-axis, E oscillates vertically, and B oscillates horizontally.

Polarization

Linear polarization: E oscillates in a single plane. Circular polarization: E traces a circle as the wave propagates — the x and y components are equal and 90° out of phase. Elliptical polarization: the general case, where the components have different amplitudes or non-90° phase difference.

Polarization filters

A polarizer transmits only the component of the E field aligned with its axis. If linearly polarized light hits a filter at angle θ to its polarization, the transmitted intensity follows Malus’s law: I = I₀ cos²(θ). At 90°, no light passes.