Let the electric field in some region $R$ be given by $\vec{E} = e^{-y^2}\hat{i} + e^{-x^2}\hat{j}$. From this we conclude that
Step 1: Use Gauss's law in differential form.
\[
\nabla \cdot \vec{E} = \frac{\rho}{\varepsilon_0}
\]
Compute divergence:
\[
\nabla \cdot \vec{E} = \frac{\partial}{\partial x}(e^{-y^2}) + \frac{\partial}{\partial y}(e^{-x^2})
\]
Both terms are nonzero because derivatives of exponentials exist.
Thus $\nabla \cdot \vec{E} \neq 0$.
Step 2: Interpretation.
If divergence is nonzero, charge density is nonzero.
Thus region contains a non-uniform charge distribution.
Step 3: Conclusion.
Correct: (A).
In a coaxial cable, the radius of the inner conductor is 2 mm and that of the outer one is 5 mm. The inner conductor is at a potential of 10 V, while the outer conductor is grounded. The value of the potential at a distance of 3.5 mm from the axis is: 
A sphere of radius \( R \) has a uniform charge density \( \rho \). A sphere of smaller radius \( \frac{R}{2} \) is cut out from the original sphere, as shown in the figure. The center of the cut-out sphere lies at \( z = \frac{R}{2} \). After the smaller sphere has been cut out, the magnitude of the electric field at \( z = -\frac{R}{2} \) is \( \frac{\rho R}{n \epsilon_0} \). The value of the integer \( n \) is: 