This can be written as:
\[ \frac{\sin(i)}{\sin(r)} = \frac{n_2}{n_1} \]
where \(i\) is the angle of incidence, \(r\) is the angle of refraction, \(n_1\) is the index of refraction of the first medium (air in this case), and \(n_2\) is the index of refraction of
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