


Concept
When unpolarized light of intensity $I_0$ passes thru a linear polarizer whose transmission axis is oriented at an angle $\theta$ relative to the transmission axis of a second linear polarizer, the transmitted intensity, $I$, is given by
$$I=I_0 \cos^2\theta$$
As the second polarizer is rotated, the transmitted intensity varies according to Malus’s Law given above. Note that as $\theta \rightarrow 90°$, $I \rightarrow 0$.
Procedure
- Place both filters parallel to each other on the overheard projector.
- Overlap the filters.
- Notice that polarized light is transmitted through each filter as well as through the combination of filters.
- Rotate one filter 90 degrees.
- Notice that the light is not transmitted through the combination of the two filters.
Equipment
- (2) Linearly Polarized Filter
- Transmission Type Overhead Projector