Mirror Mirror on the Wall - Interference Patterns · USAPhO 2020 #B2

Physics · optics

Problem

Consider a square room with side length LL. The bottom wall of the room is a perfect mirror.* A perfect monochromatic point source with wavelength λ\lambda is placed a distance dd above the center of the mirror, where λ≪d≪L\lambda \ll d \ll L. [Diagram showing a square room with side length L, point source at distance d above center of bottom mirror wall, and L/2 marked] *Remember that the phase of light reflected by a mirror changes by 180°. a. On the right wall, an interference pattern emerges. What is the distance yy between the bottom corner and the closest bright fringe above it? Hint: you may assume λ≪y≪L\lambda \ll y \ll L as well. b. You plan on running an experiment to determine λ\lambda in a room with L=40L = 40 m, and you know that λ\lambda is between 550 and 750 nm. You will measure dd and y10y_{10} (the distance of the tenth fringe from the corner) with the same ruler (with markings of 1 mm). At what dd should you place the point source to minimize your error in your λ\lambda measurement? Roughly what is that minimum error? c. Now suppose we place a transparent hemispherical shell of thickness ss and index of refraction nn over the source such that all light from the source that directly strikes the right wall passes through the shell, and all light from the source that strikes the mirror first does not pass through the shell. [Diagram showing hemispherical shell over source at distance d above mirror, with L/2 marked] At what yy is the fringe closest to the bottom-most corner now? (You may find it convenient to use ⌊x⌋\lfloor x \rfloor, the largest integer below xx.) What is the spacing between the fringes now? Ignore any reflections or diffraction from the hemispherical shell. d. Now, suppose the hemispherical shell is removed, and we instead observe the interference pattern on the top wall. To the nearest integer, what is the total number of fringes that appear on the top wall? You may assume that d≪Ld \ll L.

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