Library · Experiment
The three-polariser puzzle
Two crossed polarising filters block all light — until you slip a third one between them. A tabletop doorway into quantum measurement.
- Time
- 1 evening
- Cost
- ~£5 (polarising film)
- Difficulty
- 1 of 3
Part of Quantum from your kitchen (Light is also a particle)
The question
Two polarising filters at right angles block the light completely. How can adding a third filter — which can only block more light — make light come through again?
Learn just enough first
- Look up what polarised light is, and Malus's law, \(I = I_0 \cos^2\theta\)
- Watch a short video on the "three polariser paradox" and how it's explained with photons
Kit
- Three pieces of linear polarising film (sold cheaply in sheets online), or two pairs of polarised sunglasses and one piece of film
- A printed protractor, to set the angles
- A light source: a laptop or monitor screen (most give out polarised light), or a torch with one film in front of it
- Optional: a phone light-meter app to measure brightness
My prediction
Cross two filters so the light is blocked. If you put a third filter between them at 45°, what will happen? Write your answer down first.
Method
- Look through one filter at a white screen and rotate it. If the screen dims and brightens, the screen's light is already polarised.
- Hold two filters together and turn one until the light through them is as dark as possible. They're now crossed (90° apart).
- Slide a third filter between them and rotate it slowly. Note where it's brightest.
- Now put that third filter in front of or behind the crossed pair instead. Does it still let light through?
- With the light meter: measure brightness through two filters as you turn one from 0° to 90° in 15° steps.
Data
| Angle between two filters \(\theta\) (°) | Brightness (lux) | \(\cos^2\theta\) |
|---|---|---|
| 0 | 1.00 | |
| 15 | 0.93 | |
| 30 | 0.75 | |
| 45 | 0.50 | |
| 60 | 0.25 | |
| 75 | 0.07 | |
| 90 | 0.00 |
Result
Plot brightness against \(\cos^2\theta\): it should be close to a straight line (Malus's law). With three ideal filters at 0°, 45° and 90°, unpolarised light is halved by the first, then multiplied by \(\cos^2 45^\circ = \tfrac{1}{2}\) twice:
Real film absorbs a bit more, so expect somewhat less.
Explain it to a friend
Think of each photon as being asked a yes/no question by each filter: "are you lined up with me?" Each answer resets the photon's state. Crossed filters ask opposite questions, so nothing passes. A filter at 45° in the middle asks a different question in between, and about half the photons that get a "yes" there then have a 50:50 chance at the last filter. In quantum mechanics, measuring something changes it.
New questions
- What happens with many filters, each turned a few degrees more than the last?
- Why do polarised sunglasses cut glare from water and roads?