To solve the problem, we need to understand how intensity varies in Young's double slit experiment where there is a path difference.
The correct option is \(\frac{1}{2}\), which matches the given correct answer.
Given:
- Path difference \( \Delta x = \frac{7\lambda}{4} \).
Step 1. Calculate the phase difference \( \phi \):
\(\phi = \frac{2\pi}{\lambda} \Delta x = \frac{2\pi}{\lambda} \times \frac{7\lambda}{4} = \frac{7\pi}{2}\)
Step 2. Determine the intensity at this point:
The intensity \( I \) at a point with phase difference \( \phi \) is given by:
\(I = I_{\text{max}} \cos^2 \left(\frac{\phi}{2}\right)\)
Step 3. Calculate \( \frac{I}{I_{\text{max}}} \):
\(\frac{I}{I_{\text{max}}} = \cos^2 \left(\frac{\phi}{2}\right) = \cos^2 \left(\frac{7\pi}{4}\right)\)
Using \( \cos \frac{7\pi}{4} = \cos \left(2\pi - \frac{\pi}{4}\right) = \cos \frac{\pi}{4} \), we get:
\(\frac{I}{I_{\text{max}}} = \cos^2 \frac{\pi}{4} = \left(\frac{1}{\sqrt{2}}\right)^2 = \frac{1}{2}\)
Thus, the ratio of intensity at this point to the maximum intensity is .\( \frac{1}{2} \)
The Correct Answer is: \( \frac{1}{2} \)
A bob of mass \(m\) is suspended at a point \(O\) by a light string of length \(l\) and left to perform vertical motion (circular) as shown in the figure. Initially, by applying horizontal velocity \(v_0\) at the point ‘A’, the string becomes slack when the bob reaches at the point ‘D’. The ratio of the kinetic energy of the bob at the points B and C is: 
Two light beams fall on a transparent material block at point 1 and 2 with angle \( \theta_1 \) and \( \theta_2 \), respectively, as shown in the figure. After refraction, the beams intersect at point 3 which is exactly on the interface at the other end of the block. Given: the distance between 1 and 2, \( d = \frac{4}{3} \) cm and \( \theta_1 = \theta_2 = \cos^{-1} \left( \frac{n_2}{2n_1} \right) \), where \( n_2 \) is the refractive index of the block and \( n_1 \) is the refractive index of the outside medium, then the thickness of the block is …….. cm.

Let \( y^2 = 12x \) be the parabola and \( S \) its focus. Let \( PQ \) be a focal chord of the parabola such that \( (SP)(SQ) = \frac{147}{4} \). Let \( C \) be the circle described by taking \( PQ \) as a diameter. If the equation of the circle \( C \) is: \[ 64x^2 + 64y^2 - \alpha x - 64\sqrt{3}y = \beta, \] then \( \beta - \alpha \) is equal to: