Brewster's Angle: Reflected Light Perfectly Polarized
1 · Predict
At one special angle of incidence (Brewster's angle), light reflecting off a surface becomes perfectly polarized — the reflected beam contains only one polarization direction. Does a higher-index surface have a larger or smaller Brewster angle?
- Larger — a higher refractive index requires a steeper incidence angle to satisfy the Brewster condition.
- A higher index gives a smaller Brewster angle.
- Brewster's angle doesn't depend on the surface's index.
2 · Set Up
- Open the brewster preset and press Reset. Light travels from air (n₁ = 1.0) toward glass.
- Enable the Brewster-angle readout.
- Set the glass's refractive index for each trial and record the Brewster angle.
3 · Collect Data
| Glass index n₂ | Brewster angle θ_B (°) |
|---|---|
| 1.33 | |
| 1.5 | |
| 1.7 |
Plot θ_B (y-axis) against n₂ (x-axis) for your three trials.
4 · Analyze
- For one trial, compute θ_B = atan(n₂/n₁) using n₁ = 1.0. Compare to the table.
- Explain why a higher-index surface (n₂ larger) requires a LARGER Brewster angle — steeper incidence — to achieve perfectly polarized reflection.
5 · Extend
- At Brewster's angle, reflected glare (like off a lake or wet road) is almost entirely horizontally polarized. This is exactly why polarized sunglasses (blocking horizontal polarization) are so effective at cutting glare — they're tuned to block precisely the light that's most strongly reflected at typical viewing angles.
- At Brewster's angle, the reflected beam contains ZERO p-polarized light (polarized in the plane of incidence) — only s-polarized light reflects. Explain why this means a camera with a polarizing filter, rotated to block s-polarized light, can nearly eliminate reflections off glass or water at this specific angle.
The Physics Behind This Experiment
Brewster's Angle
At the specific incidence angle θ_B = atan(n₂/n₁), reflected light becomes perfectly polarized (purely s-polarized, with the reflected and refracted rays at exactly 90° to each other). This is the physical basis for polarized anti-glare sunglasses and camera filters.