A parallel beam of light of intensity $I_0$ is incident on a glass plate, $25 \%$ of light is reflected by…
- $\left[\frac{\frac{1}{2}+\sqrt{\frac{3}{8}}}{\frac{1}{2}-\sqrt{\frac{3}{8}}}\right]^2$
- $\left[\frac{\frac{1}{4}+\sqrt{\frac{3}{8}}}{\frac{1}{2}-\sqrt{\frac{3}{8}}}\right]^2$
- $\frac{5}{8}$
- $\frac{8}{5}$
Solution

Given that, $25 \%$ of total intensity of incident light is reflected from upper surface. This implies, if intensity of incident light is $\mathrm{I}_0$, the intensity of light reaching the lower surface of plate will be $\frac{3}{4} \mathrm{I}_0$. As $50 \%$ of this intensity is reflected, the final intensity of light emerging from glass plate will be $\frac{3}{8} \mathrm{I}_0$. $\begin{aligned} \therefore \quad I_1 & =\frac{I_0}{4} \\ & I_2=\frac{3}{8} I_0 \end{aligned}$ Now, $\frac{I_{\max }}{I_{\min }}=\frac{\left(\sqrt{I_1}+\sqrt{I_2}\right)^2}{\left(\sqrt{I_1}-\sqrt{I_2}\right)^2}=\left(\frac{\frac{1}{2}+\sqrt{\frac{3}{8}}}{\frac{1}{2}-\sqrt{\frac{3}{8}}}\right)^2$
Asked in: MHT CET 2024 (04 May Shift 2)