The body is released from rest from the top of a tower.
So initial velocity is:
\[
u=0.
\]
Let the height of the tower be:
\[
H.
\]
The total time to reach the ground is:
\[
T.
\]
Using the equation of motion:
\[
s=ut+\frac{1}{2}gt^2.
\]
Since \(u=0\),
\[
s=\frac{1}{2}gt^2.
\]
For the complete fall:
\[
H=\frac{1}{2}gT^2.
\]
Now, at time:
\[
t=\frac{T}{2},
\]
distance fallen from the top is:
\[
s=\frac{1}{2}g\left(\frac{T}{2}\right)^2.
\]
\[
s=\frac{1}{2}g\cdot \frac{T^2}{4}.
\]
\[
s=\frac{1}{8}gT^2.
\]
But from total height:
\[
H=\frac{1}{2}gT^2.
\]
So,
\[
\frac{1}{8}gT^2=\frac{1}{4}\left(\frac{1}{2}gT^2\right).
\]
\[
s=\frac{H}{4}.
\]
This is the distance fallen from the top.
Therefore, the distance of the body from the ground is:
\[
H-\frac{H}{4}.
\]
\[
=\frac{3H}{4}.
\]
Hence, at time \(T/2\), the body is:
\[
\frac{3H}{4}
\]
above the ground.