Step 1: Substitute the given constants.
The potential is $\phi(x,y,z) = \phi_0 \frac{x_0}{x}$. With $\phi_0 = 8\,\text{V}$ and $x_0 = 5\,\text{m}$:
\[
\phi = \frac{8 \times 5}{x} = \frac{40}{x}
\]
Step 2: Recognise that the potential depends only on x.
Since $\phi$ does not depend on $y$ or $z$, the electric field has no $y$ or $z$ components.
Only $E_x$ is non-zero.
Step 3: Use the relation $E_x = -d\phi/dx$.
\[
E_x = -\frac{d\phi}{dx} = -\frac{d}{dx}\left(\frac{40}{x}\right) = -\left(-\frac{40}{x^2}\right) = \frac{40}{x^2}
\]
Step 4: Evaluate at the given point $(10\,\text{m},5\,\text{m},5\,\text{m})$.
Only $x = 10\,\text{m}$ matters:
\[
E_x = \frac{40}{10^2} = \frac{40}{100} = 0.40\,\text{V\,m}^{-1}
\]
Step 5: Write the complete electric field vector.
\[
\vec{E} = 0.40\,\hat{i}\,\text{V\,m}^{-1}
\]
The field points in the positive $x$-direction because the potential decreases as $x$ increases (higher $x$, lower $\phi$).
Step 6: State the answer.
\[
\boxed{0.40\,\text{V\,m}^{-1}\,\hat{i}}
\]