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Polarization

Light is a transverse electromagnetic wave and can be polarized — meaning its electric field oscillates in a definite direction. Polarizers, Brewster angles, and birefringent materials allow precise control of polarization state.

Key Concepts

  • Malus's law: I = I₀cos²θ
  • Brewster's angle: tanθ_B = n₂/n₁
  • Birefringent materials have two refractive indices (ordinary and extraordinary)
  • Quarter-wave plates convert linear to circular polarization
  • Unpolarized light through one polarizer: I = I₀/2

Key Equations

Malus's law
I=I0cos2θI = I_0\cos^2\theta
Brewster's angle
tanθB=n2n1\tan\theta_B = \frac{n_2}{n_1}
Phase retardation
δ=2πλ(neno)d\delta = \frac{2\pi}{\lambda}(n_e - n_o)d
Quarter-wave plate
δ=π2d=λ4(neno)\delta = \frac{\pi}{2} \Rightarrow d = \frac{\lambda}{4(n_e - n_o)}
Worked Example

Example Problem

Problem

Find Brewster's angle for light going from air (n=1) into glass (n=1.5).

Solution

tanθ_B = n₂/n₁ = 1.5/1 → θ_B = arctan(1.5) = 56.3°.

Practice

Exercises

7 problems
1 of 7

Unpolarized light (I₀=100 W/m²) passes through a polarizer. Find the transmitted intensity in W/m².

W/m²
2 of 7

Linearly polarized light (100 W/m²) passes through a polarizer at 45°. Find the transmitted intensity using Malus's law.

W/m²
3 of 7

Find Brewster's angle (degrees) for light going from water (n=1.33) into glass (n=1.5).

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4 of 7

Polarized light passes through two polarizers: first at 30°, second at 90° relative to initial polarization. Find the final intensity if I₀=200 W/m².

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5 of 7

A quarter-wave plate for λ=600 nm uses a crystal with |nₑ-nₒ|=0.009. Find the required thickness in μm.

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6 of 7

At what analyzer angle θ would the transmitted intensity be I₀/4 (I₀ is incident polarized intensity)?

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7 of 7

Light (I₀=160 W/m²) passes through 3 polarizers at 0°, 30°, 60°. Find final intensity in W/m².

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Key Takeaways

  • Malus's law I = I₀cos²θ governs transmission through an analyzer
  • Brewster's angle produces completely polarized reflected light
  • Birefringent plates control the relative phase of polarization components
  • Combining polarizers in sequence multiplies the cosine-squared transmission factors