Concept:
- Trace the ray step by step through the prism using the refraction angle at each surface, instead of jumping straight to the formula. This makes it clear why $r=A/2$ and $i=(A+\delta_m)/2$ hold at minimum deviation.
Step 1: Set up the two refracting surfaces.
A prism has two surfaces meeting at angle $A = 60^\circ$. The ray refracts once entering (angle $r_1$) and once leaving (angle $r_2$), with $r_1 + r_2 = A$.
Step 2: Use the symmetry of minimum deviation.
At minimum deviation, the ray inside the prism runs parallel to the base, which forces $r_1 = r_2$. Combined with $r_1+r_2=60^\circ$, this gives $r_1 = r_2 = 30^\circ$.
Step 3: Find the incidence angle from the total deviation.
Total deviation $\delta_m = (i_1 - r_1) + (i_2 - r_2)$. Since $i_1 = i_2 = i$ and $r_1=r_2=r$ at minimum deviation, this becomes $\delta_m = 2i - 2r + (r_1+r_2) - (r_1+r_2)$, which simplifies to $\delta_m = 2i - A$.
So $i = \dfrac{\delta_m+A}{2} = \dfrac{30^\circ+60^\circ}{2} = 45^\circ$.
Step 4: Apply Snell's law at the point of entry.
$\mu = \dfrac{\sin i}{\sin r_1} = \dfrac{\sin 45^\circ}{\sin 30^\circ} = \dfrac{\sqrt{2}/2}{1/2} = \sqrt{2}$
Final Answer: $\mu = \sqrt{2}$