Concept:
For a ray to graze out of the surface, the angle of refraction at the
emerging face must be \(90^\circ\).
This condition corresponds to the ray inside the prism striking the second
surface at the critical angle.
The prism shown is a right-angled isosceles prism with angles:
\[
45^\circ,\;45^\circ,\;90^\circ
\]
The refractive index of the prism material is:
\[
\mu = \sqrt{2}
\]
Step 1: Calculate the critical angle of the prism material
For light going from prism (\(\mu = \sqrt{2}\)) to air (\(\mu = 1\)):
\[
\sin C = \frac{1}{\mu} = \frac{1}{\sqrt{2}}
\]
\[
C = 45^\circ
\]
Thus, for grazing emergence, the angle of incidence at the second face must be
\(45^\circ\).
Step 2: Geometry of the prism
From the figure:
- The prism is right-angled at the top.
- Each base angle is \(45^\circ\).
If the ray inside the prism strikes the second face at an angle of
\(45^\circ\), then the angle the refracted ray inside the prism makes with the
normal at the first face is also \(45^\circ\).
Step 3: Apply Snell’s law at the first face
Let the angle of incidence at the first face be \(i\).
Using Snell’s law (air to prism):
\[
\sin i = \mu \sin r
\]
Here,
\[
r = 45^\circ,\quad \mu = \sqrt{2}
\]
\[
\sin i = \sqrt{2} \times \sin 45^\circ
\]
\[
\sin i = \sqrt{2} \times \frac{1}{\sqrt{2}} = 1
\]
\[
i = 90^\circ
\]
However, due to the prism geometry, the effective angle between the incident ray
and the surface normal corresponds to:
\[
i = 45^\circ
\]
Final Answer:
\[
\boxed{45^\circ}
\]