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Question

Two polarisers $P_1$ and $P_2$ are placed in such a way that the intensity of the transmitted light will be zero. A third polariser $P_3$ is inserted in between $P_1$ and $P_2$, at particular angle between $P_2$ and $P_3$. The transmitted intensity of the light passing the through all three polarisers is maximum. The angle between the polarisers $P_2$ and $P_3$ is :

The correct answer is
$\frac{\pi}{4}$

Polariser Intensity Problem Setup

We are given three polarisers, $P_1$, $P_3$, and $P_2$. Initially, $P_1$ and $P_2$ are oriented such that the transmitted light intensity between them is zero. This implies their transmission axes are perpendicular.

Let the angle of the transmission axis of $P_1$ be $\alpha_1 = 0$. Then, the angle of the transmission axis of $P_2$ is $\alpha_2 = \frac{\pi}{2}$ (or $90^\circ$).

Calculating Maximum Transmitted Intensity

A third polariser, $P_3$, is placed between $P_1$ and $P_2$. Let its transmission axis be at an angle $\theta$ relative to $P_1$. Thus, its angle is $\alpha_3 = \theta$.

The intensity $I$ after passing through all three polarisers, starting from unpolarized light of initial intensity $I_{unpol}$, is given by:

$I = I_{unpol} \cos^2(\alpha_3 - \alpha_1) \cos^2(\alpha_2 - \alpha_3)$

Substituting the angles:

$I = I_{unpol} \cos^2(\theta - 0) \cos^2(\frac{\pi}{2} - \theta)$

Using the identity $\cos(\frac{\pi}{2} - \theta) = \sin(\theta)$, the expression becomes:

$I = I_{unpol} \cos^2(\theta) \sin^2(\theta)$

Finding the Angle for Maximum Intensity

To maximize the transmitted intensity $I$, we need to maximize the term $\cos^2(\theta) \sin^2(\theta)$.

We can rewrite this term using the double angle identity $\sin(2\theta) = 2\sin(\theta)\cos(\theta)$:

$\cos^2(\theta) \sin^2(\theta) = (\cos(\theta)\sin(\theta))^2 = \left(\frac{\sin(2\theta)}{2}\right)^2 = \frac{1}{4} \sin^2(2\theta)$

The intensity is:

$I = I_{unpol} \frac{1}{4} \sin^2(2\theta)$

This intensity is maximum when $\sin^2(2\theta)$ is maximum, which is 1.

$\sin^2(2\theta) = 1$

This occurs when $2\theta = \frac{\pi}{2}$. Solving for $\theta$ gives:

$\theta = \frac{\pi}{4}$

This angle $\theta = \frac{\pi}{4}$ is the angle of $P_3$ relative to $P_1$. The question asks for the angle between polarisers $P_2$ and $P_3$.

Determining the Angle Between $P_2$ and $P_3$

The angle between $P_2$ and $P_3$ is $|\alpha_2 - \alpha_3|$.

Angle = $|\frac{\pi}{2} - \theta| = |\frac{\pi}{2} - \frac{\pi}{4}| = \frac{\pi}{4}$.

Therefore, the angle between the polarisers $P_2$ and $P_3$ is $\frac{\pi}{4}$.

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