The body slides down a smooth inclined plane from rest.
For motion from rest with constant acceleration:
\[
s=\frac{1}{2}at^2.
\]
This means:
\[
s\propto t^2.
\]
Let the total length of the inclined plane be:
\[
L.
\]
The time taken to slide the full length \(L\) is:
\[
T=4\text{ sec}.
\]
So,
\[
L=\frac{1}{2}aT^2.
\]
Now, let the time taken to slide \(\frac{1}{4}\) of the length be \(t\).
Then:
\[
\frac{L}{4}=\frac{1}{2}at^2.
\]
Now divide this equation by the full-length equation:
\[
\frac{\frac{L}{4}}{L}=\frac{\frac{1}{2}at^2}{\frac{1}{2}aT^2}.
\]
Cancel common terms:
\[
\frac{1}{4}=\frac{t^2}{T^2}.
\]
Taking square root:
\[
\frac{1}{2}=\frac{t}{T}.
\]
Therefore:
\[
t=\frac{T}{2}.
\]
Since
\[
T=4\text{ sec},
\]
we get:
\[
t=\frac{4}{2}=2\text{ sec}.
\]
Hence, the required time is:
\[
2\text{ sec}.
\]