(c) Electric field
$E = - \frac{d\phi}{dt} = - 2ar$
By Gauss’s theorem
$E\left( 4\pi r^{2} \right) = \frac{q}{\varepsilon_{0}}$
$q = - 8\pi\varepsilon_{0}{ar}^{2}$
$\rho = \frac{dq}{dV} = \frac{dq}{dr} \times \frac{dr}{dV}$
$= \left( - 24\pi\varepsilon_{0}ar^{2} \right) \times \frac{1}{4\pi r^{2}}$
$\rho = - 6\varepsilon_{0}a$