In this case, the refractive index of air is 1 and the refractive index of glass is n. So, we have:
\[n_1 \sin(\theta_i) = n_2 \sin(\theta_r)\]
where \(n_1\) is the refractive index of air, \(\theta_i\) is the angle of incidence, \(n_2\) is the refractive index
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