law

Malus's law

Malus's law describes how the intensity of polarized light transmitted through a polarizer varies with the cosine squared of the angle between the light's polarization and the polarizer's axis.
23 related articles · 3 formulas · 1 who worked here

Description

In 1809, French officer Étienne Louis Malus, looking through a crystal of Iceland spar at the reflection of the setting sun in the windows of the Luxembourg Palace, noticed something astonishing: as he rotated the crystal, the reflection alternately faded and brightened. He realized that reflected light was no longer chaotic but preferred one direction of vibration, and he called this polarization. Passing such light through a second crystal, Malus derived a strict relationship: intensity I depends on the angle θ as I = I₀cos²θ. Today, a simple turn of the head in sunglasses or the motion of a pixel on a screen are governed by this cosine. Malus's law became the first quantitative conquest of polarization optics and proved the transverse nature of light waves.

History

Étienne Louis Malus, an officer in the Napoleonic army and engineer, was studying birefringence in crystals in 1809. One evening, while looking through a crystal at the sunset reflection in the Luxembourg Palace, he was surprised to notice that one of the two images disappeared when rotating the crystal. Thus, the phenomenon of polarization by reflection was discovered. Malus measured how brightness changed and derived the relation: intensity is proportional to the square of the cosine of the angle. The law confirmed the transverse nature of light waves and became part of the toolkit of optics. Later, Augustin Fresnel provided a theoretical justification within the wave theory.

How it works

Malus's law works for fully polarized light and an ideal dichroic analyzer. It underlies the operation of polarimeters, LCD displays, polarizing filters in photography, and is also applied in polarization microscopy and in studies of optically active substances. Limitations: it does not hold for partially polarized light — a statistical generalization is required; in real materials, there are always small losses and depolarization.

In practice

In LCD screens, each pixel is a tiny liquid-crystal shutter that, on command, rotates the polarization, adjusting brightness strictly according to Malus's law. Polarizing sunglasses quench glare on water, glass, and wet asphalt because reflected light is polarized horizontally, while the glasses are oriented vertically — angle 90°, light does not pass.

Fun fact

Light from the blue sky is polarized: if you look at a patch at 90° to the sun through a polarizer and rotate it, the sky noticeably darkens — a direct consequence of Malus's law. Bees and ants use the same trick for navigation.

Concept graph →

Formulas

$$L = 4\pi R^2 \sigma T^4$$
Luminosity relates to radius and temperature.
What is in the formula
LvariableLuminosity (total power radiated) — luminosity watt
RvariableRadius of the radiating body — radius metre
TvariableEffective temperature of the surface — temperature kelvin
\sigmaconstantProportionality constant relating blackbody radiated power to temperature — stefan boltzmann constant = 5.670374419e-8 watt per metre squared per kelvin to the fourth
r=\sqrt{\frac{l}{4πσt^4}} · 2606.06575v1
l=4πr^2σt^4 · 2606.28993
l=4πr^2σt^4 · 2606.29435
l=4πr^2σt^4 · 2607.06684
$$T(R) \propto R^{-\alpha}$$
Temperature varies with radius as a power law.
What is in the formula
Tvariabletemperature — temperature kelvin
Rvariableradius (distance from center) — radius metre
αvariablepower-law index (positive for decreasing temperature outward)
t(r)=120{k}(r/{au})^{-3/7} · 2607.02660v1
$$I = I_0 e^{-\sigma n x}$$
Intensity decreases exponentially with absorber column density.
What is in the formula
IvariableTransmitted intensity — intensity watt per square metre
I_0variableIncident intensity — intensity watt per square metre
σvariableAbsorption cross-section per absorber — cross section square metre
nvariableNumber density of absorbers — number density per cubic metre
xvariablePath length through the medium — length metre
\phi=\phi_0e^{-σ(e)n_ax},\quadx=\int_0^lρ(l)dl · 2607.02644

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