Step 1: Resolve the velocity into horizontal and vertical components.
The ball strikes the horizontal ground with speed
\[
u=5\,\text{m s}^{-1}
\]
at an angle
\[
30^\circ
\]
with the horizontal.
Horizontal component:
\[
u_x=u\cos30^\circ
\]
\[
u_x=5\left(\frac{\sqrt3}{2}\right)
\]
\[
u_x=\frac{5\sqrt3}{2}
\]
Vertical component (towards the ground):
\[
u_y=u\sin30^\circ
\]
\[
u_y=5\left(\frac12\right)
\]
\[
u_y=\frac52
\]
Step 2: Apply coefficient of restitution.
For collision with a smooth horizontal ground, the horizontal component remains unchanged.
Therefore,
\[
v_x=\frac{5\sqrt3}{2}
\]
The vertical component after collision becomes
\[
v_y=e\,u_y
\]
where
\[
e=0.2=\frac15
\]
Hence,
\[
v_y=\frac15\cdot\frac52
\]
\[
v_y=\frac12
\]
and its direction is upward.
Step 3: Find the speed after reflection.
The speed of the reflected ball is
\[
v=\sqrt{v_x^2+v_y^2}
\]
\[
v=\sqrt{\left(\frac{5\sqrt3}{2}\right)^2+\left(\frac12\right)^2}
\]
\[
v=\sqrt{\frac{75}{4}+\frac14}
\]
\[
v=\sqrt{\frac{76}{4}}
\]
\[
v=\sqrt{19}
\]
Step 4: Final conclusion.
Therefore, the speed of the reflected ball is
\[
\boxed{\sqrt{19}\,\text{m s}^{-1}}
\]