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).
Match List-I with List-II.
Choose the correct answer from the options given below :}
There are three co-centric conducting spherical shells $A$, $B$ and $C$ of radii $a$, $b$ and $c$ respectively $(c>b>a)$ and they are charged with charges $q_1$, $q_2$ and $q_3$ respectively. The potentials of the spheres $A$, $B$ and $C$ respectively are:
Two resistors $2\,\Omega$ and $3\,\Omega$ are connected in the gaps of a bridge as shown in the figure. The null point is obtained with the contact of jockey at some point on wire $XY$. When an unknown resistor is connected in parallel with $3\,\Omega$ resistor, the null point is shifted by $22.5\,\text{cm}$ towards $Y$. The resistance of unknown resistor is ___ $\Omega$. 
