Step 1: Write the relation between electric field and potential.
Electric field is related to electric potential by
\[
\vec{E}=-\nabla \phi
\]
Given,
\[
\phi(x,y,z)=\phi_0\frac{x_0}{x}
\]
Substituting
\[
\phi_0=8\,V
\]
and
\[
x_0=5\,m,
\]
we get
\[
\phi=\frac{8\times 5}{x}
\]
\[
\phi=\frac{40}{x}
\]
Step 2: Differentiate the potential with respect to \(x\).
Since the potential depends only on \(x\),
\[
E_x=-\frac{d\phi}{dx}
\]
Now,
\[
\frac{d\phi}{dx}=\frac{d}{dx}\left(\frac{40}{x}\right)
\]
\[
\frac{d\phi}{dx}=-\frac{40}{x^2}
\]
Therefore,
\[
E_x=-\left(-\frac{40}{x^2}\right)
\]
\[
E_x=\frac{40}{x^2}
\]
Hence,
\[
\vec{E}=\frac{40}{x^2}\hat{i}
\]
Step 3: Evaluate the electric field at \(x=10\,m\).
At the point
\[
(10\,m,5\,m,5\,m),
\]
we have
\[
x=10\,m
\]
So,
\[
\vec{E}=\frac{40}{(10)^2}\hat{i}
\]
\[
\vec{E}=\frac{40}{100}\hat{i}
\]
\[
\vec{E}=0.40\,Vm^{-1}\hat{i}
\]
Step 4: Final conclusion.
Hence, the electric field at the given point is
\[
\boxed{0.40\,Vm^{-1}\,\hat{i}}
\]