Step 1: Find the vertical fall on the inclined plane.
Highest point height:
\[
8.75\,\text{m}
\]
Lowest point height:
\[
3.75\,\text{m}
\]
So, vertical fall is
\[
8.75-3.75=5\,\text{m}
\]
Step 2: Find the velocity at the lower edge.
Using conservation of energy,
\[
mgh=\frac{1}{2}mv^2
\]
\[
v^2=2gh
\]
\[
v^2=2(10)(5)=100
\]
\[
v=10\,\text{m/s}
\]
Step 3: Resolve velocity components.
The sphere leaves the roof at an angle \(30^\circ\) below the horizontal.
Horizontal component:
\[
u_x=10\cos30^\circ=10\cdot \frac{\sqrt{3}}{2}=5\sqrt{3}
\]
Vertical downward component:
\[
u_y=10\sin30^\circ=10\cdot \frac{1}{2}=5
\]
Step 4: Find time to reach the ground.
The sphere falls from height
\[
3.75\,\text{m}
\]
Using
\[
s=u_yt+\frac{1}{2}gt^2
\]
\[
3.75=5t+5t^2
\]
\[
5t^2+5t-3.75=0
\]
Solving,
\[
t=\frac{1}{2}\,\text{s}
\]
Step 5: Find horizontal distance.
Horizontal distance is
\[
R=u_xt
\]
\[
R=5\sqrt{3}\times \frac{1}{2}
\]
\[
R=\frac{5\sqrt{3}}{2}\,\text{m}
\]
Step 6: Final conclusion.
Hence,
\[
\boxed{\frac{5\sqrt{3}}{2}\,\text{m}}
\]