p35 015


15. The water is medium1, so n1 = nw which we simply write as n. The air is medium2, for which n2 H" 1.
We refer points where the light rays strike the water surface as A (on the left side of Fig. 35-32) and B
(on the right side of the picture). The point midway between A and B (the center point in the picture) is
C. The penny P is directly below C, and the location of the  apparent or Virtual penny is V . We note

that the angle CV B (the same as CV A) is equal to ¸2, and the angle CP B (the same as CP A) is
equal to ¸1. The triangles CV B and CP B share a common side, the horizontal distance from C to B
(which we refer to as x). Therefore,
x x
tan ¸2 = and tan ¸1 = .
da d
Using the small angle approximation (so a ratio of tangents is nearly equal to a ratio of sines) and the
law of refraction, we obtain
tan ¸2 sin ¸2
H"
tan ¸1 sin ¸1
x
n1
da
H"
x
n2
d
d
H" n
da
which yields the desired relation: da = d/n.


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