Step 1:
We start by applying Snell's law at the first interface (air-quartz), which gives us:
\[n_{1} \sin(\theta_{1}) = n_{2} \sin(\theta_{2})\]
where $n_{1}$ is the refractive index of air, $\theta_{1}$ is the angle of incidence, $n_{2}$ is the refractive index
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