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(For sound, c is usually taken to be the speed of sound in air, so that n for sound is often < 1.)
Note that for refraction from a medium of greater index of refraction into a medium with a lesser index of refraction (n1 > n2),
there are angles θ1 > θcritical for which there is no solution:
Reflection results in a phase change of π when it is off the surface of a medium with a higher index of refraction.
Refraction
n ≡ c / v.
Note that the frequency is unchanged as light moves through different mediums.
n1 sin θ1 = n2 sin θ2,
where θi are measured relative to the normal to the interface between the media:
n1 sin θcritical = n2.
These angles result in total internal reflection back into the original medium.
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©2010, Kenneth R. Koehler. All Rights Reserved. This document may be freely reproduced provided that this copyright notice is included.
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