Pasco OS-8520 PHOTOMETER Manuel d'utilisateur Page 4

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Photometer 012-05631A
Experiment 2: Polarization
Polarized
Light
Unpolarized
Light
First Polarizer
No Light
Second Polarizer
Figure 2.1: Unpolarized light incident on two polarizers
oriented perpendicularly to each other.
First Polarizer
Unpolarized
Light
Polarized
Light
Polarized
Light
φ
I = I
o
cos
2
φ
I
o
φ
Second Polarizer
Figure 2.2: Unpolarized light incident on two polarizers
oriented at an angle φ with respect to each other.
EQUIPMENT NEEDED
– Optics bench (OS-8518) – 2 Point light sources (OS-8517)
– Photometer with filter set (OS-8520) – 2 Polarizers (OS-8520)
Purpose
The purpose of this experiment is to show that the intensity of the light transmitted through two
polarizers depends on the square of the cosine of the angle between the axes of the two
polarizers.
Theory
A polarizer only allows light which is vibrating in a particular plane to pass through it. This
plane forms the “axis” of polarization. Unpolarized light vibrates in all planes. Thus if unpolar-
ized light is incident upon an “ideal” polarizer, only half will be transmitted through the
polarizer. (Since in reality no polarizer is “ideal”, less than half the light will be transmitted.)
The transmitted light is polarized in one plane. If this polarized light is incident upon a second
polarizer, the axis of which is oriented such that it is perpendicular to the plane of polarization
of the incident light, no light will be transmitted through the second polarizer (Figure 2.1).
However, if the second polarizer is oriented at an angle so that it is not perpendicular to the first
polarizer, there will be some component of the electric field of the polarized light that lies in the
same direction as the axis of the second polarizer, and thus some light will be transmitted
through the second polarizer (Figure 2.2).
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