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Optics}Polarizers

When one has three polarizers with the first oriented at a 90 degree angle to the last, the maximum light transmitted is I_0/8.

In this case, the intensity of light transmitted through the first filter is I_0/2, where I_0 is the incident light. (Half the light has been canceled by the polarization.)

The intensity of the light transmitted through the second filter is I_2 = |I_1 \cos 45^\circ|^2 = I_0/4.

The intensity of the light transmitted through the third filter is I_3 = |I_2 \cos 45^\circ|^2 = I_0/8.

This is choice (B).

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Comments
jmason86
2009-07-03 14:27:44
Conceptually this is really weird.
The first filter cuts the light in half, which makes sense. You could imagine that all the light is now, say, vertical.
The second filter is at 45 degrees, but the light is already vertical, so this should just reduce the intensity.
The last filter is at 90 degrees from the first, so it should only allow horizontal light through, but there is none... it's all vertical. So I would expect no light to be transmitted through this filter.

The math works out fine, but I cant imagine how this works physically.
kroner
2009-10-06 14:57:02
One way to think about it is in terms of photon spin. If you have an ensemble of photons in a pure vertical spin state and you measure the spin in the 45 degree orientation, the act of measuring messes up the vertical/horizontal state. After that if you measure the vertical/horizontal orientation you'll get half and half.
NEC
Richard
2007-10-25 22:41:25
This is another instance of Malus' Law:

When you have polarized light I_0
through a polarizer at an angle \theta,
I_0\cos^2 (\theta) gets through.

How to get the first 1/2:
Initially, however, the light is unpolarized.
You might just realize that 1/2 of the unpolarized light gets through, but a more justifiable approach is to
imagine a superposition of light more or less polarized equally at every possible angle (unpolarized light):
Apply Malus' Law to this situation and you get
\frac{I_0}{N}cos^2 (\theta_1)+\frac{I_0}{N}cos^2 (\theta_2)+...\frac{I_0}{N}cos^2 (\theta_N) which is nothing more than the average of \cos^2(\theta)=1/2.
NEC
antithesis
2007-10-01 13:26:55
I understand the math here, but intuitively, something seems off:

If you were to take out the second polarizer, the 3rd would be 90 degrees from the first, and you would get
I_1 = \frac{1}{2}I_0 and I_2 = I_1 cos^2 ( 90 ) = 0.

So how come adding the second polarizer now allows light to go through?
irishroogie
2007-10-02 11:22:33
You have to consider the angle between the 2nd and the 3rd polarizer which is 45 degrees.
f4hy
2009-04-02 16:50:57
Yes this is the mystery of it. It seems like light should not make it through but it does!
NEC
Andresito
2006-03-08 22:10:28
Intensity is not squared but only the cosine function. Otherwise the dimensions would not be correct.

Thanks for working out the solutions Yosun :p
Typo Alert!
kk7t
2005-12-10 11:25:41
there should be a square on I1, I2.NEC

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