In a YDSE, the light of wavelength $I=5000\,�$ is used, which emerges in phase from two slits a distance $d=3 \times 10^{-7} m$ apart. A transparent sheet of thickness $t=1.5 \times 10^{-7} m$ refractive index $\mu=1.17$ is placed over one of the slits. what is the new angular position of the central maxima of the interference pattern, from the center of the screen? Find the value of $y$.
The path difference when transparent sheet is introduced $\Delta x=(\mu-1) t$ If the central maxima occupies position of nth fringe ,then $(\mu-1) t=n \lambda=d \sin \theta$ $\Rightarrow \sin \theta=\frac{(\mu-1) t}{d}$ $=\frac{(1.17-1) \times 1.5 \times 10^{-7}}{3 \times 10^{-7}}=0.085$ Therefore, angular position of central maxima $\theta=\sin ^{-1}(0.085)=4.88^{\circ} \approx 4.9$ For For small angles, $\sin \theta \approx \theta \approx \tan \theta$ $\Rightarrow \tan \theta=\frac{y}{D}$ $\therefore \frac{y}{D} =\frac{(\mu-1) t}{d}$ $\Rightarrow y=\frac{D(\mu-1) t}{D}$
Considering two waves interfering at point P, having different distances. Consider a monochromatic light source ‘S’ kept at a relevant distance from two slits namely S1 and S2. S is at equal distance from S1 and S2. SO, we can assume that S1 and S2 are two coherent sources derived from S.
The light passes through these slits and falls on the screen that is kept at the distance D from both the slits S1 and S2. It is considered that d is the separation between both the slits. The S1 is opened, S2 is closed and the screen opposite to the S1 is closed, but the screen opposite to S2 is illuminating.
Thus, an interference pattern takes place when both the slits S1 and S2 are open. When the slit separation ‘d ‘and the screen distance D are kept unchanged, to reach point P the light waves from slits S1 and S2 must travel at different distances. It implies that there is a path difference in the Young double-slit experiment between the two slits S1 and S2.