Solution to 1992 Problem 64


Recall Maxwell's equations:
\begin{align*}\nabla \cdot \mathbf{E} &= \frac{1}{\epsilon_0}\rho \\\nabla \times \mathbf{E} &= -\frac{\partial \math...
If you plug the given electric field into Gauss's Law, you will find that
\begin{align*}k = \frac{1}{\epsilon_0}\rho\end{align*}
We are told that k is a nonzero constant. Therefore, \rho must also be nonzero, and so there must be charge density in the region. Therefore, answer (B) is correct.


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