Step 1: In Young's double slit experiment, the intensity of light at a point is given by: \[ I = I_0 \cos^2 \left( \frac{\pi \Delta x}{\lambda} \right) \] where \( \Delta x \) is the path difference, and \( \lambda \) is the wavelength. If the path difference is \( \frac{\lambda}{3} \), the intensity can be calculated by substituting the value of the path difference: \[ I = I_0 \cos^2 \left( \frac{\pi \times \frac{\lambda}{3}}{\lambda} \right) = I_0 \cos^2 \left( \frac{\pi}{3} \right) = I_0 \left( \frac{1}{2} \right)^2 = \frac{I_0}{4} \] Thus, the intensity at the point with path difference \( \frac{\lambda}{3} \) is \( \boxed{\frac{I}{4}} \). \bigskip
If the monochromatic source in Young's double slit experiment is replaced by white light,
1. There will be a central dark fringe surrounded by a few coloured fringes
2. There will be a central bright white fringe surrounded by a few coloured fringes
3. All bright fringes will be of equal width
4. Interference pattern will disappear