A ray is incident from a medium of refractive index \(2\) into a medium of refractive index \(1\). The critical angle is
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Critical angle exists only when light travels from a denser medium to a rarer medium. The formula is:
\[
\sin C=\frac{n_2}{n_1}
\]
where \(n_1\gt n_2\).
Step 1: Recognise the situation. Light goes from a denser medium ($n_1 = 2$) into a rarer medium ($n_2 = 1$). When light moves dense to rare, total internal reflection becomes possible beyond a special angle called the critical angle. Step 2: Apply Snell's law at the critical angle. At the critical angle $C$, the refracted ray grazes along the boundary, so the angle of refraction is $90^\circ$: \[ n_1\sin C = n_2\sin 90^\circ. \] Step 3: Simplify. Since $\sin 90^\circ = 1$, \[ \sin C = \frac{n_2}{n_1}. \] Step 4: Substitute the indices. \[ \sin C = \frac{1}{2}. \] Step 5: Find the angle. \[ C = \sin^{-1}\!\left(\frac{1}{2}\right) = 30^\circ. \] Step 6: Conclude. Thus the critical angle for this pair of media is $30^\circ$. \[ \boxed{30^\circ} \]
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