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: \( \frac{1}{2} \)
Consider the sound wave travelling in ideal gases of $\mathrm{He}, \mathrm{CH}_{4}$, and $\mathrm{CO}_{2}$. All the gases have the same ratio $\frac{\mathrm{P}}{\rho}$, where P is the pressure and $\rho$ is the density. The ratio of the speed of sound through the gases $\mathrm{v}_{\mathrm{He}}: \mathrm{v}_{\mathrm{CH}_{4}}: \mathrm{v}_{\mathrm{CO}_{2}}$ is given by