p34 036

background image

36. As the unpolarized beam of intensity I

0

passes the first polarizer, its intensity is reduced to

1
2

I

0

. After

passing through the second polarizer, for which the direction of polarization is at an angle θ from that
of the first one, the intensity is I =

1
2

I

0

cos

2

θ =

1
3

I

0

. Thus, cos

2

θ = 2/3, which leads to θ = 35

.


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