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[link] shows the effect of two polarizing filters on originally unpolarized light. The first filter polarizes the light along its axis. When the axes of the first and second filters are aligned (parallel), then all of the polarized light passed by the first filter is also passed by the second. If the second polarizing filter is rotated, only the component of the light parallel to the second filter’s axis is passed. When the axes are perpendicular, no light is passed by the second.
Only the component of the EM wave parallel to the axis of a filter is passed. Let us call the angle between the direction of polarization and the axis of a filter . If the electric field has an amplitude , then the transmitted part of the wave has an amplitude (see [link] ). Since the intensity of a wave is proportional to its amplitude squared, the intensity of the transmitted wave is related to the incident wave by
where is the intensity of the polarized wave before passing through the filter. (The above equation is known as Malus’s law.)
What angle is needed between the direction of polarized light and the axis of a polarizing filter to reduce its intensity by ?
Strategy
When the intensity is reduced by , it is or 0.100 times its original value. That is, . Using this information, the equation can be used to solve for the needed angle.
Solution
Solving the equation for and substituting with the relationship between and gives
Solving for yields
Discussion
A fairly large angle between the direction of polarization and the filter axis is needed to reduce the intensity to of its original value. This seems reasonable based on experimenting with polarizing films. It is interesting that, at an angle of , the intensity is reduced to of its original value (as you will show in this section’s Problems&Exercises). Note that is from reducing the intensity to zero, and that at an angle of the intensity is reduced to of its original value (as you will also show in Problems&Exercises), giving evidence of symmetry.
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