Derivation of Refractive Index of the Prism 
When a ray of light is incident normally on a refracting face of a prism, the angle of incidence $i = 0$, and the ray enters the prism without deviation. Inside the prism, the ray undergoes refraction at the second face, resulting in a total deviation angle $\delta$. Using the geometry of the prism: \[ \delta = i_e - i_r, \] where: $i_e$ is the angle of emergence, $i_r$ is the angle of refraction inside the prism. From Snell's law at the second face: \[ n = \frac{\sin i_e}{\sin i_r}. \] At the point of minimum deviation ($\delta = \delta_m$), the angles of incidence and emergence are equal: \[ i_e = A + \frac{\delta}{2}. \] Substituting: \[ n = \frac{\sin(A + \delta)}{\sin A}. \] Thus, the refractive index of the prism is: \[ \boxed{n = \frac{\sin(A + \delta)}{\sin A}}. \]
Two slits 0.1 mm apart are arranged 1.20 m from a screen. Light of wavelength 600 nm from a distant source is incident on the slits. How far apart will adjacent bright interference fringes be on the screen?

A ladder of fixed length \( h \) is to be placed along the wall such that it is free to move along the height of the wall.
Based upon the above information, answer the following questions:
(iii) (b) If the foot of the ladder, whose length is 5 m, is being pulled towards the wall such that the rate of decrease of distance \( y \) is \( 2 \, \text{m/s} \), then at what rate is the height on the wall \( x \) increasing when the foot of the ladder is 3 m away from the wall?