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Q.In Young's double slit experiment, the separation between the two slits is halved. The new fringe width will be __________ times its initial value.

CBSECBSE Class XII Board 2020Subjective· 1mImportance★★★★★
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Fringe width in YDSE is inversely proportional to slit separation; halving the slit separation doubles the fringe width. The new value is 2 times the initial value.

Why Optical Path Difference Controls the Fringes

In Young’s double slit experiment, the entire pattern — bright and dark bands — arises from the path difference between light waves arriving from the two slits. When the slits are separated by distance dd, the path difference at a point on the screen at angle θ\theta is dsin⁡θd \sin \theta. For small angles (which is the usual case in YDSE), sin⁡θ≈tan⁡θ=y/D\sin \theta \approx \tan \theta = y/D, where yy is the distance from the central maximum and DD is the slit-to-screen distance.

The fringe width β\beta is the distance between two consecutive bright (or dark) fringes. It comes directly from the condition for constructive interference: dsin⁡θ=nλd \sin \theta = n\lambda. Changing dd changes how quickly the path difference varies with position, which in turn changes how closely the fringes are spaced.

β=λDd\beta = \frac{\lambda D}{d}

This is the central result: fringe width depends inversely on slit separation dd, and directly on wavelength λ\lambda and screen distance DD.


Step-by-step reasoning

1. Write the standard expression for fringe width

For small angles, the fringe width in YDSE is:

β=λDd\beta = \frac{\lambda D}{d}

where λ\lambda is the wavelength of light, DD is the distance from slits to screen, and dd is the separation between the two slits.

2. Identify what changes and what stays constant

The problem states that the slit separation is halved. So the new separation is:

d′=d2d' = \frac{d}{2}

The wavelength λ\lambda and the screen distance DD remain unchanged — they are properties of the light source and the experimental setup, not affected by moving the slits closer together. …

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