In this case, the first medium is air and the second medium is the glass block. So, we have:
\[n_1 \sin(\theta_1) = n_2 \sin(\theta_2)\]
where \(n_1 = 1\) (refractive index of air), \(\theta_1 = 30^\circ\) (angle of incidence), \(n_2 = 1.5\) (refractive index of
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