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The directions and three problems from examination 4 of the university of california, berkeley's physics 110b spring 2004 course. The problems involve topics such as wave interference, thin slits, and refraction. Students are required to solve the problems using given information and show their work. No calculators or laptops are allowed, but they may use a bluebook and their own original handwriting.
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University of California, Berkeley Physics 110B Spring 2004 (Strovink)
EXAMINATION 4
Directions: Do all three problems, which have unequal weight. This is a closed-book closed-note examexcept for Griffiths, Pedrotti, a copy of anything posted on the course web site, and anything in your own original handwriting (not Xeroxed). Calculators are not needed, but you may use one if you wish. Laptops and palmtops should be turned off. Use a bluebook. Do not use scratch paper – otherwise you risk losing part credit. Show all your work. Cross out rather than erase any work that you wish the grader to ignore. Justify what you do. Express your answer in terms of the quantities specified in the problem. Box or circle your answer.
Problem 1. (20 points) A plane wave of initial irradiance I 0 propagat- ing along ˆz is incident upon a screen lying in the z = 0 plane. The screen is totally absorbing, except that one quadrant of it (the piece with 0 < x, y < ∞) is missing. An observer stationed at (0, 0 , z), where kz 1, detects an irradiance I′. What is I′/I 0 , and why?
Problem 2. (40 points) (a.) (20 points) Consider four equally spaced long (∆y = ∞) thin slits, located in the z = 0 plane at x = ± d 2
and x = ± 32 d. As usual, tan ψx = dxdz of the out- going wavefront. Consider the aperture function for these four slits to be the convolution of a pair of δ-functions separated by d and another pair of δ-functions separated by 2d (both pairs are symmetric about x = 0). In the Fraunhofer limit, write down the irradiance pattern
R(ψx) ≡
I(ψx) I(ψx = 0)
as the product of two two-slit R’s.
(b.) (20 points) Consider an opaque baffle in the z = 0 plane in which a 4×4 array of 16 tiny holes is drilled. The holes are arranged on a square grid, with verti- cal and horizontal hole-to-hole separation equal to d. The entire array is centered at the origin (where there is no hole). In the Fraunhofer limit, defining tan ψx = dxdz and tan ψy = dydz of the out- going wavefront, deduce the resulting irradiance
pattern
R(ψx, ψy ) ≡
I(ψx, ψy ) I(ψx = 0, ψy = 0)
Please justify your answer.
Problem 3. (40 points) A monochromatic beam traveling in medium “0” is normally incident upon a substrate “T”. Three films (“1”, “2”, and “3”) are interposed between the two media, such that film 1 adjoins medium 0 and film 3 adjoins medium T. The refractive indices are frequency-independent and equal, respectively, to n 0 , n 1 , n 2 , n 3 , and nT , with n 0 = nT. You may assume that all mate- rials are insulating and nonabsorbing, and that they all have the same magnetic permeability. Films “1” and “3” have thickness λi/4 (where λi is the wavelength of the beamin the partic- ular material of which that film is made), while film“2” has thickness λi/2.
(a.) (20 points) Work out a condition on n 0 , n 1 , n 2 , n 3 , and nT that allows no light to be reflected.
(b.) (20 points) Now the frequency of the monochromatic beam is doubled (red light becomes blue light), while all three films retain their same physical thick- nesses (in meters). As a function of the (unre- stricted) five refractive indices, what is the ratio R of the reflected to incident irradiance?