Concept:
For a light ray to retrace its original path after reflecting from a surface (the silvered second face of the prism), it must strike that surface normally (perpendicularly). This means the angle of incidence at the second surface is $0^\circ$. We can then use the prism geometry equations ($A = r_1 + r_2$) and Snell's Law to find the refractive index.
Step 1: Identify the angles at the two surfaces.
Let the angle of incidence at the first surface be $i = 2A$.
Let the angle of refraction at the first surface be $r_1$.
Let the angle of incidence at the second (silvered) surface be $r_2$.
Because the ray retraces its path, it must hit the silvered surface at exactly $90^\circ$ to the surface, which means the angle with the normal is zero:
$$r_2 = 0^\circ$$
Step 2: Find the angle of refraction $r_1$.
The refracting angle of a prism ($A$) is related to the internal angles by:
$$A = r_1 + r_2$$
Substitute $r_2 = 0$:
$$A = r_1 + 0 \implies r_1 = A$$
Step 3: Apply Snell's Law at the first surface.
Snell's Law states $\mu_1 \sin i = \mu_2 \sin r$. Assuming the prism is in the air ($\mu_1 = 1$), the refractive index of the prism ($\mu$) is:
$$\mu = \frac{\sin i}{\sin r_1}$$
Substitute $i = 2A$ and $r_1 = A$:
$$\mu = \frac{\sin(2A)}{\sin A}$$
Step 4: Simplify using trigonometric identities.
Use the double angle identity $\sin(2A) = 2 \sin A \cos A$:
$$\mu = \frac{2 \sin A \cos A}{\sin A}$$
Cancel out $\sin A$:
$$\mu = 2 \cos A$$