To solve this problem, we need to analyze the refraction of light through an equilateral prism with a refractive index \( \sqrt{2} \) and determine the angle of refraction at the incident surface when the emergent ray grazes along the second surface. Let's break down the solution into steps:
Understanding the Setup: We have an equilateral prism, meaning all angles are \(60^\circ\). The refractive index of the prism is \( \sqrt{2} \). A light ray is incident on one of its faces at an angle \( i \).
Condition for Grazing Emergence: For a ray to graze along the surface, the angle of emergence must be \(90^\circ\). By applying Snell's Law at the emergent surface, where the angle of refraction is \(90^\circ\), we get:
\(n \sin(r_2) = 1 \cdot \sin(90^\circ)\)
Since \(\sin(90^\circ) = 1\), then \(n \sin(r_2) = 1\).
Thus, \(\sin(r_2) = \frac{1}{n} = \frac{1}{\sqrt{2}}\).
This implies \( r_2 = 45^\circ \).
Application of Geometry of the Prism: For an equilateral prism:
\(A + \delta = (r_1 + r_2)\) and \( A = 60^\circ \) because it's an equilateral prism.
Thus, \(60^\circ = r_1 + 45^\circ \), which solves to \( r_1 = 15^\circ \).
Conclusion: The angle of refraction \( r_1 \) at the incident surface is \(15^\circ\).
Finally, we can verify \( r_1 = 15^\circ \) using Snell's Law:
\(n_1 \sin(i) = n_2 \sin(r_1)\), where \(n_1 = 1\) (air) and \(n_2 = \sqrt{2}\).
So, \(\sin(i) = \sqrt{2} \cdot \sin(15^\circ)\). But since exact \( i \) was not asked, the question verifies for \( r_1 \).
Therefore, the correct answer is \(15^\circ\).