In Young’s double slit experimental set-up, the intensity of the central maximum is \( I_0 \). Calculate the intensity at a point where the path difference between two interfering waves is \( \frac{\lambda}{3} \).
The intensity in Young’s double slit experiment is given by:
\[ I = I_0 \cos^2\left( \frac{\pi \Delta x}{\lambda} \right) \]
Where:
- \( I_0 \) is the intensity of the central maximum,
- \( \Delta x \) is the path difference between the two waves,
- \( \lambda \) is the wavelength of the light.
Given: \( \Delta x = \frac{\lambda}{3} \), we substitute into the equation:
\[ I = I_0 \cos^2\left( \frac{\pi}{3} \right) \]
Since \( \cos\left( \frac{\pi}{3} \right) = \frac{1}{2} \), we get:
\[ I = I_0 \left( \frac{1}{2} \right)^2 = \frac{I_0}{4} \]
Final Answer:
The intensity at the point where the path difference is \( \frac{\lambda}{3} \) is: \[ I = \frac{I_0}{4} \]
Light from a point source in air falls on a spherical glass surface (refractive index, \( \mu = 1.5 \) and radius of curvature \( R = 50 \) cm). The image is formed at a distance of 200 cm from the glass surface inside the glass. The magnitude of distance of the light source from the glass surface is 1cm.

