When light is incident normally on a refracting face of the prism, the deviation \( \delta \) is related to the prism angle \( A \) and the refractive index \( n \) as follows:
The angle of incidence on the first face is \( 0^\circ \), and hence the refraction occurs only at the second face of the prism.
The angle of refraction \( r_2 \) at the second face satisfies Snell's Law:
\[ n = \frac{\sin(i_2)}{\sin(r_2)} \]
where \( i_2 \) is the angle of incidence at the second face. Since the total deviation \( \delta \) is given by:
\[ \delta = i_2 + r_1 - A \]
and for normal incidence, \( r_1 = 0 \), we have:
\[ \delta = i_2 - A \quad \text{or} \quad i_2 = \delta + A \]
Substituting \( i_2 = \delta + A \) into Snell's Law:
\[ n = \frac{\sin(\delta + A)}{\sin A} \]
Hence, the refractive index of the prism material is:
\[ n = \frac{\sin(\delta + A)}{\sin A} \]