A monochromatic and linearly polarised light is used in a Young's double slit experiment. A linear polarizer, whose pass axis is at an angle $45^\circ$ to the polarization of the incident wave, is placed in front of one of the slits. If $I_{max}$ and $I_{min}$, respectively, denote the maximum and minimum intensities of the interference pattern on the screen, the visibility, defined as the ratio $\frac{I_{max} - I_{min}}{I_{max} + I_{min}}$ is
$\frac{2}{3}$
This problem calculates the visibility of an interference pattern in a Young's double-slit experiment where a linear polarizer affects the light intensity and polarization for one slit.
The incident light is monochromatic and linearly polarized. Let its initial intensity be $I_0$ and its polarization direction be $\hat{p}_1$.
The visibility ($V_{std}$) is fundamentally related to the intensities ($I_1, I_2$) of the waves contributing to the interference:
$V_{std} = \frac{I_{max} - I_{min}}{I_{max} + I_{min}} = \frac{2 \sqrt{I_1 I_2}}{I_1 + I_2}$
Substitute the intensities $I_1 = I_0$ and $I_2 = \frac{1}{2} I_0$ into the formula:
$V_{std} = \frac{2 \sqrt{I_0 \cdot \frac{1}{2} I_0}}{I_0 + \frac{1}{2} I_0} = \frac{2 \sqrt{\frac{1}{2} I_0^2}}{\frac{3}{2} I_0} = \frac{2 \cdot \frac{1}{\sqrt{2}} I_0}{\frac{3}{2} I_0}$
Simplifying this expression gives:
$V_{std} = \frac{\sqrt{2} I_0}{\frac{3}{2} I_0} = \frac{2\sqrt{2}}{3}$
The polarizer alters the polarization state. The light from slit 1 has polarization $\hat{p}_1$, and from slit 2 has polarization $\hat{p}_2$, with an angle of $45^\circ$ between them. The factor representing this mismatch is $|\hat{p}_1 \cdot \hat{p}_2| = \cos(45^\circ) = \frac{1}{\sqrt{2}}$.
The effective visibility ($V$) accounts for this polarization difference:
$V = V_{std} |\hat{p}_1 \cdot \hat{p}_2|$
Substituting the calculated $V_{std}$ and the polarization mismatch factor:
$V = \frac{2\sqrt{2}}{3} \cdot \frac{1}{\sqrt{2}} = \frac{2}{3}$
The resulting visibility of the interference pattern is $\frac{2}{3}$.
A screen has two slits, each of width $w$, with their centres at a distance $2w$ apart. It is illuminated by a monochromatic plane wave travelling along the $x$-axis.

The intensity of the interference pattern, measured on a distant screen, at an angle $\theta = n\lambda/w$ to the $x$-axis is
A film projector and microscope give equal magnification. But a film projector is not used to see living cells because
A pair of parallel glass plates separated by a distance $d$ is illuminated by white light as shown in the figure below. Also shown is the graph of the intensity of the reflected light $I$ as a function of the wavelength $\lambda$ recorded by a spectrometer.
Assuming that the interference takes place only between light reflected by the bottom surface of the top plate and the top surface of bottom plate, the distance $d$ is closest to