This was rightly taken note of by the Nobel Committee. Since the interval BC is common to both triangles, we easily see that sin(θI ) λI =. (3.1) λR sin(θR ) Since λI = cI T = cvac T /nI and λR = cR T = cvac T /nR where cI and cR are the wave speeds to the left and right of the interface, cvac is the speed of light in a vacuum, and T is the (common) period, we can easily recast the above equation in the form nI sin(θI ) = nR sin(θR ). (3.2) This is called Snell’s law, and it governs how a ray of light bends as it passes through a discontinuity in the index of refraction.

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