Step 1: Recall the equation of motion.
For a body moving with uniform acceleration:
\[
s = ut + \frac{1}{2}at^2
\]
Step 2: Use the condition “starts from rest”.
If the body starts from rest:
\[
u = 0
\]
So the equation reduces to:
\[
s = \frac{1}{2}at^2
\]
Step 3: Identify the relation between \( s \) and \( t \).
From the equation:
\[
s \propto t^2
\]
Step 4: Interpret physically.
With constant acceleration, displacement increases quadratically with time.
Step 5: Check dimensions.
Since
\[
[a]=LT^{-2}
\]
we get
\[
s \sim at^2 \sim L
\]
which is consistent.
Step 6: Verify with an example.
If \( t \) doubles:
\[
s \propto t^2 \Rightarrow s \text{ becomes } 4 \text{ times}
\]
which matches uniformly accelerated motion.
Step 7: Final conclusion.
Hence,
\[
\boxed{s \propto t^2}
\]
Therefore, the correct option is
\[
\boxed{(4)\ s \propto t^2}
\]