The fringe width \( \beta \) in Young's double slit experiment is given by: \[ \beta = \frac{\lambda D}{d} \] where \( \lambda \) is the wavelength of light, \( D \) is the distance between the slits and the screen, and \( d \) is the distance between the slits. When the experiment is performed in a medium with refractive index \( \mu \), the wavelength of light changes. The wavelength of light in a medium is given by: \[ \lambda_{\text{medium}} = \frac{\lambda}{\mu} \] Thus, the fringe width in the liquid becomes: \[ \beta_{\text{liquid}} = \frac{\lambda_{\text{medium}} D}{d} = \frac{\lambda D}{\mu d} = \frac{\beta}{\mu} \] When the experiment is returned to air (with refractive index \( \mu = 1 \)), the fringe width will be multiplied by \( \mu \).Therefore, the fringe width in air will be: \[ \mu \beta \]
Thus, the correct answer is (D): \( \mu \beta \).
The fringe width (\(\beta\)) in Young's double slit experiment is given by:
\(\beta = \frac{\lambda D}{d}\)
where:
When the setup is immersed in a liquid of refractive index \(\mu\), the wavelength of light changes to \(\lambda' = \frac{\lambda}{\mu}\). The new fringe width \(\beta'\) is given as \(\beta\).
\(\beta = \frac{\lambda' D}{d} = \frac{\lambda D}{\mu d}\)
When the experiment is performed in air (refractive index = 1), let the fringe width be \(\beta_{air}\). Then:
\(\beta_{air} = \frac{\lambda D}{d}\)
From the first equation, we have:
\(\beta = \frac{\beta_{air}}{\mu}\)
Therefore,
\(\beta_{air} = \mu \beta\)
So the fringe width in air is \(\mu\beta\).
Therefore, the answer is \(\mu\beta\).
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: