We know that the intensity at a point in Young's double-slit experiment is given by:
\[
I = I_0 \cos^2 \left( \frac{\pi \Delta}{\lambda} \right),
\]
where \( I_0 \) is the maximum intensity and \( \Delta \) is the path difference.
For path difference \( \Delta = \lambda \), the intensity is \( K \). Thus, we have:
\[
K = I_0 \cos^2 \left( \pi \right) = I_0.
\]
Now, for the path difference \( \Delta = \lambda / 6 \), we calculate the intensity:
\[
I = I_0 \cos^2 \left( \frac{\pi}{6} \right) = I_0 \times \left( \frac{\sqrt{3}}{2} \right)^2 = \frac{3}{4} I_0.
\]
Since \( K = I_0 \), the intensity at a point where the path difference is \( \lambda / 6 \) is:
\[
I = \frac{3}{4} K.
\]