The fringe width in the Young's double slit experiment is given by the formula: \[ \beta = \frac{\lambda D}{d} \] Where: - \( \beta \) is the fringe width, - \( \lambda \) is the wavelength of the light, - \( D \) is the distance between the screen and the slits, - \( d \) is the separation between the slits.
When the apparatus is immersed in a liquid of refractive index \( n \), the wavelength of the light in the liquid becomes \( \lambda' = \frac{\lambda}{n} \).
Thus, the new fringe width \( \beta' \) will be: \[ \beta' = \frac{\lambda' D}{d} = \frac{\frac{\lambda}{n} D}{d} = \frac{\lambda D}{n d} = \frac{\beta}{n} \] Given:
- Initial fringe width \( \beta = 2.6 \, \text{mm} \),
- Refractive index \( n = 1.3 \).
Now, calculating the new fringe width: \[ \beta' = \frac{2.6}{1.3} = 2 \, \text{mm} \] Thus, the new fringe width is \( 2 \, \text{mm} \).
If the ratio of lengths, radii and Young's Moduli of steel and brass wires in the figure are $ a $, $ b $, and $ c $ respectively, then the corresponding ratio of increase in their lengths would be:
Two charges $ -q $ each are fixed, separated by distance $ 2d $. A third charge $ q $ of mass $ m $ placed at the mid-point is displaced slightly by $ x' (x \ll d) $ perpendicular to the line joining the two fixed charges as shown in the figure. The time period of oscillation of $ q $ will be: