Step 1: Trace the path of the ray of light through the prism. When a ray of light enters a prism with refractive index greater than that of the surrounding medium (typically air), it bends towards the normal at the first interface (at angle of incidence \(i\)), passes through the prism, and bends away from the normal at the second interface (at angle of exit \(e\)). The prism has an apex angle \(A\).
Step 2: Derive the formula for the angle of deviation (\(\delta\)). The angle of deviation (\(\delta\)) is the angle by which the light ray deviates from its original direction after passing through the prism. It can be expressed in terms of the angle of incidence (\(i\)), the angle of exit (\(e\)), and the prism's apex angle (\(A\)) as follows: \[ \delta = i + e - A \] This relationship arises because the external deviation is equal to the sum of the angles of incidence and emergence minus the angle of the prism.
Step 3: Graph the variation of \(\delta\) with \(i\). The relationship between \(\delta\) and \(i\) is typically non-linear, showing that \(\delta\) decreases with an increase in \(i\) up to a minimum value (at the minimum deviation condition) and then increases. The graph of \(\delta\) versus \(i\) will have a "U" shape, indicating the minimum deviation occurs when the light ray passes symmetrically through the prism.
When light travels from an optically denser medium to an optically rarer medium, at the interface it is partly reflected back into the same medium and partly refracted to the second medium. The angle of incidence corresponding to an angle of refraction 90° is called the critical angle (ic) for the given pair of media. This angle is related to the refractive index of medium 1 with respect to medium 2. Refraction of light through a prism involves refraction at two plane interfaces. A relation for the refractive index of the material of the prism can be obtained in terms of the refracting angle of the prism and the angle of minimum deviation. For a thin prism, this relation reduces to a simple equation. Laws of refraction are also valid for refraction of light at a spherical interface. When an object is placed in front of a spherical surface separating two media, its image is formed. A relation between object and image distance, in terms of refractive indices of two media and the radius of curvature of the spherical surface can be obtained. Using this relation for two surfaces of lens, ’lensemaker formula’ is obtained.
