The source emits unpolarised light, and the given intensity ratio is:
\[ r = \frac{I_A}{I_B} = 2 \]
When the first polaroid is introduced, the intensity of light becomes:
\[ I'_B = \frac{I_B}{2} \]
When the second polaroid is introduced at 45° relative to the first, the intensity of light becomes:
\[ I''_B = I'_B \cdot \cos^2(45^\circ) = \frac{I_B}{2} \cdot \frac{1}{2} = \frac{I_B}{4} \]
The new intensity ratio is:
\[ r' = \frac{I_A}{I''_B} = \frac{I_A}{\frac{I_B}{4}} = 4 \cdot \frac{I_A}{I_B} = 4 \times 2 = 8 \]
r = 8
To solve the problem, analyze the intensity changes due to distance and polaroids.
Given:
- Point source \(S\) emits unpolarized light uniformly.
- Intensity ratio at points \(A\) and \(B\):
\[
r = \frac{I_A}{I_B} = 2
\]
- Two polaroids with 45° angle between their pass-axes are placed before point \(B\).
Step 1: Intensity ratio without polaroids:
Since source is uniform and unpolarized, intensity decreases with distance squared:
\[
I \propto \frac{1}{d^2}
\]
Thus,
\[
\frac{I_A}{I_B} = \frac{d_B^2}{d_A^2} = 2
\]
or equivalently,
\[
\frac{I_B}{I_A} = \frac{1}{2}
\]
Step 2: Effect of two polaroids on intensity:
- First polaroid reduces intensity of unpolarized light by half:
\[
I' = \frac{I_B}{2}
\]
- Second polaroid at angle \(\theta = 45^\circ\) passes intensity according to Malus's law:
\[
I'' = I' \cos^2 45^\circ = \frac{I_B}{2} \times \left(\frac{1}{\sqrt{2}}\right)^2 = \frac{I_B}{2} \times \frac{1}{2} = \frac{I_B}{4}
\]
Step 3: New intensity at point B after polaroids:
\[
I_B' = \frac{I_B}{4}
\]
Step 4: New ratio \(r'\) of intensities at \(A\) and \(B\):
\[
r' = \frac{I_A}{I_B'} = \frac{I_A}{I_B / 4} = 4 \times \frac{I_A}{I_B} = 4 \times 2 = 8
\]
Final Answer:
\[
\boxed{8}
\]
The center of a disk of radius $ r $ and mass $ m $ is attached to a spring of spring constant $ k $, inside a ring of radius $ R>r $ as shown in the figure. The other end of the spring is attached on the periphery of the ring. Both the ring and the disk are in the same vertical plane. The disk can only roll along the inside periphery of the ring, without slipping. The spring can only be stretched or compressed along the periphery of the ring, following Hooke’s law. In equilibrium, the disk is at the bottom of the ring. Assuming small displacement of the disc, the time period of oscillation of center of mass of the disk is written as $ T = \frac{2\pi}{\omega} $. The correct expression for $ \omega $ is ( $ g $ is the acceleration due to gravity): 
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