To solve this problem, we need to understand the effect of introducing a glass plate in one of the paths of the interfering beams in Young's Double Slit Experiment.
In Young's Double Slit Experiment, the condition for maxima (bright fringes) is given by the equation:
\(d \sin \theta = n \lambda\)
where \(d\) is the slit separation, \(\theta\) is the angle of diffraction, \(n\) is the order of the maximum, and \(\lambda\) is the wavelength of light.
When a glass plate of thickness \(t\) and refractive index \(\mu\) is introduced in the path of one of the beams, it introduces an additional phase difference. The optical path length in the medium of refractive index \(\mu\) is given by:
\(OP = \mu t\)
The introduction of the glass plate shifts the path difference by:
\(\Delta = (\mu - 1) t\)
For the central maximum to remain unchanged, the path difference due to the glass plate should be an integral multiple of the wavelength:
\((\mu - 1) t = m \lambda\)
Since the intensity at the central maximum remains unchanged, \(m = 1\). Therefore:
\((\mu - 1) t = \lambda\)
Given that the thickness of the glass plate is \(t = x \lambda\), substituting this into the equation, we have:
\((\mu - 1) x \lambda = \lambda\)
Simplifying this gives:
\(x = \frac{1}{\mu - 1}\)
For the given refractive index \(\mu = 1.5\),
\(x = \frac{1}{1.5 - 1} = \frac{1}{0.5} = 2\)
The value of \(x\) is therefore 2.
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