KCET · Physics · Ray Optics
A ray of light enters from a rarer to a denser medium. The angle of incidence is Then the reflected and refracted rays are mutually perpendicular to each other. The critical angle for the pair of media is
- A \(\sin ^{-1}(\tan \mathrm{i})\)
- B \(\tan ^{-1}(\sin \mathrm{i})\)
- C \(\sin ^{-1}(\cot \mathrm{i})\)
- D \(\cos ^{-1}(\tan \mathrm{i})\)
Answer & Solution
Correct Answer
(C) \(\sin ^{-1}(\cot \mathrm{i})\)
Step-by-step Solution
Detailed explanation
From law of reflection, \(\angle \mathrm{i}=\angle \mathrm{r}\) and
\(
\frac{\sin \mathrm{r}^{\prime}}{\sin \mathrm{i}}=\frac{\mu_{\mathrm{d}}}{\mu_{\mathrm{r}}}
\)
From the figure

\(
r^{\prime}=\left(90^{\circ}-i\right)
\)
From Eq. (ii) \(\frac{\sin \left(90^{\circ}-i\right)}{\sin i}=\frac{\mu_{\mathrm{d}}}{\mu_{\mathrm{r}}}\) or \(\quad \frac{\cos \mathrm{i}}{\sin \mathrm{i}}=\frac{\mu_{\mathrm{d}}}{\mu_{\mathrm{r}}} \Rightarrow \cot \mathrm{i}=\frac{\mu_{\mathrm{d}}}{\mu_{\mathrm{r}}}\)
But \(\frac{\mu_{\mathrm{d}}}{\mu_{\mathrm{r}}}=\sin \mathrm{C}\) (where is critical angle) \(\therefore \quad \cot \mathrm{i}=\sin \mathrm{C} \Rightarrow \mathrm{C}=\sin ^{-1}(\cot \mathrm{i})\)
\(
\frac{\sin \mathrm{r}^{\prime}}{\sin \mathrm{i}}=\frac{\mu_{\mathrm{d}}}{\mu_{\mathrm{r}}}
\)
From the figure

\(
r^{\prime}=\left(90^{\circ}-i\right)
\)
From Eq. (ii) \(\frac{\sin \left(90^{\circ}-i\right)}{\sin i}=\frac{\mu_{\mathrm{d}}}{\mu_{\mathrm{r}}}\) or \(\quad \frac{\cos \mathrm{i}}{\sin \mathrm{i}}=\frac{\mu_{\mathrm{d}}}{\mu_{\mathrm{r}}} \Rightarrow \cot \mathrm{i}=\frac{\mu_{\mathrm{d}}}{\mu_{\mathrm{r}}}\)
But \(\frac{\mu_{\mathrm{d}}}{\mu_{\mathrm{r}}}=\sin \mathrm{C}\) (where is critical angle) \(\therefore \quad \cot \mathrm{i}=\sin \mathrm{C} \Rightarrow \mathrm{C}=\sin ^{-1}(\cot \mathrm{i})\)
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