To solve this problem, we need to understand how the angular width of the first minima in a double-slit experiment changes when the medium is changed from air to water.
The angular width of the first minima for a double-slit experiment is given by the formula:
\(\theta = \frac{\lambda}{d}\)
Where:
When the setup is immersed in water, the effective wavelength (\(\lambda_{\text{effective}}\)) of light in the medium changes according to the refractive index (\(\mu\)) of the medium:
\(\lambda_{\text{effective}} = \frac{\lambda}{\mu}\)
Given:
In water, the effective wavelength of light is:
\(\lambda_{\text{water}} = \frac{400 \, \text{nm}}{\frac{4}{3}} = 300 \, \text{nm}\)
Therefore, the new angular width of the first minima, \(\theta_{\text{water}}\), is:
\(\theta_{\text{water}} = \theta_{\text{air}} \times \frac{\lambda_{\text{water}}}{\lambda}\)
Plugging in the values:
\(\theta_{\text{water}} = 0.2^\circ \times \frac{300 \, \text{nm}}{400 \, \text{nm}} = 0.15^\circ\)
Therefore, the angular width of the first minima when the setup is immersed in water is 0.15^\circ.
Thus, the correct answer is 0.15°.