Step 1: Understand the interference pattern equation.
In Young's double slit experiment, the intensity at a point on the screen is given by the equation:
\[
I = I_{\text{max}} \cos^2 \left( \frac{\pi \Delta x}{\lambda} \right)
\]
where \( I_{\text{max}} \) is the maximum intensity, \( \Delta x \) is the path difference, and \( \lambda \) is the wavelength of the light.
Step 2: Use the given intensity ratio.
The problem states that the intensity is \( \frac{3}{4} \) of the maximum intensity, so:
\[
\frac{I}{I_{\text{max}}} = \frac{3}{4}
\]
Thus, we have the equation:
\[
\cos^2 \left( \frac{\pi \Delta x}{\lambda} \right) = \frac{3}{4}
\]
Step 3: Solve for the path difference.
Taking the square root of both sides:
\[
\cos \left( \frac{\pi \Delta x}{\lambda} \right) = \frac{\sqrt{3}}{2}
\]
The cosine value of \( \frac{\sqrt{3}}{2} \) corresponds to \( \frac{\pi}{6} \), so:
\[
\frac{\pi \Delta x}{\lambda} = \frac{\pi}{6}
\]
Step 4: Find \( x \).
Solving for \( \Delta x \):
\[
\Delta x = \frac{\lambda}{6}
\]
Since \( \Delta x = \frac{\lambda}{x} \), we conclude:
\[
\frac{\lambda}{x} = \frac{\lambda}{6}
\]
Thus, the value of \( x \) is:
\[
x = 6
\]