Polarization

Polarization describes the orientation of a transverse wave's oscillation. For light, it is conventionally defined by the direction of the electric field. Polarizers make that orientation measurable and controllable.

What it means for light to be polarized

Unpolarized light and linearly polarized light after a polarizer many transverse orientations polarizer axis one linear polarization remains
Polarization reveals the transverse character of electromagnetic waves. A linear polarizer selects the electric-field component along its transmission axis.

Unpolarized light contains rapidly varying transverse orientations. Linearly polarized light has a definite electric-field direction. Longitudinal sound in air does not have this same polarization degree of freedom.

An ideal linear polarizer

An ideal polarizer transmits the electric-field component along its axis. For unpolarized input, the average transmitted intensity after the first ideal polarizer is I = Iunpol/2.

Two polarizer axes separated by an angle theta first polarization direction θanalyzer axisI = I₀ cos² θ for already polarized input
Malus's law depends on the angle between polarization direction and analyzer axis. Parallel axes transmit maximum intensity; ideal crossed axes give zero.

Malus's law

I = I₀ cos² θ

I₀ is the intensity of light already polarized before the analyzer; θ is the angle between that polarization and the analyzer axis.

Malus-law explorer

0°

Do not automatically apply the one-half factor again if I₀ already describes polarized light incident on the analyzer.

Reflection can polarize light

Reflection from nonmetallic surfaces often favors one polarization, which is why polarized sunglasses can reduce glare from roads and water. At Brewster's angle, the reflected and refracted rays are perpendicular and the reflected light is ideally fully polarized in one orientation.

Real polarizers absorb and scatter some light, so measured transmission is not perfectly ideal.

Three checks before using Malus's law

First identify whether the incident light is already polarized. Second identify the polarization direction immediately before the analyzer. Third measure θ between that direction and the analyzer axis. Only then apply I = I₀ cos²θ.

If the starting light is unpolarized and ideal, the first polarizer gives half the incident intensity on average; Malus's law then applies to subsequent analyzers. Real materials have finite transmission and imperfect extinction, so laboratory values need not reach the ideal 0 or 100% limits.

Worked examples

1. Malus at 60°

Linearly polarized light of intensity 80 W m−2 reaches an analyzer at 60°. Find transmitted intensity.

Solution

I = I₀ cos²60° = 80(0.5)² = 20 W m−2.

2. Unpolarized first polarizer

Ideal unpolarized light of intensity 100 W m−2 passes through one ideal polarizer. What is the average transmitted intensity?

Solution

An ideal first polarizer transmits half the unpolarized intensity on average: 50 W m−2.

3. Two ideal crossed polarizers

Linearly polarized light is aligned with the first polarizer, and a second ideal polarizer is at 90°. What does Malus’s law predict?

Solution

I = I₀ cos²90° = 0 in the ideal model.