Concept:
In projectile motion, the horizontal component of velocity remains constant throughout the motion. The minimum speed occurs at the highest point where vertical velocity becomes zero.
Thus:
\[
v_{\min}=u\cos\theta
\]
Given:
\[
u\cos\theta = 40
\]
Also,
\[
x = (u\cos\theta)t
\]
\[
y = (u\sin\theta)t - \frac12 gt^2
\]
Step 1: Use the displacement ratio condition.
At \(t=2\,\text{s}\),
\[
\frac{y}{x}=\frac{1}{2}
\]
Now,
\[
x=(u\cos\theta)(2)
\]
\[
=40\times2
\]
\[
=80\,\text{m}
\]
Vertical displacement:
\[
y=(u\sin\theta)(2)-\frac12(10)(2)^2
\]
\[
=2u\sin\theta-20
\]
Using ratio:
\[
\frac{2u\sin\theta-20}{80}=\frac12
\]
Step 2: Solve for \(u\sin\theta\).
\[
2u\sin\theta-20=40
\]
\[
2u\sin\theta=60
\]
\[
u\sin\theta=30
\]
Step 3: Find angle of projection.
We already know:
\[
u\cos\theta=40
\]
Hence,
\[
\tan\theta=\frac{30}{40}
\]
\[
=\frac34
\]
Using \(3-4-5\) triangle:
\[
\sin\theta=\frac35=0.6
\]
Therefore,
\[
\boxed{\theta=\sin^{-1}(0.6)}
\]