Say for the sake of this question we have a microscopic 3D sphere of radius $r$. This disk has a charge $q$ which is uniformly distributed.
What is the electric field within the sphere? Does it vary as a function of radius?
Edit: I've spent of bit of time on this over the last few days, trying to extend the approach that Griffiths used for point charges to this system. If there's an error in this approach please let me know.
The flux of $E$ through an enclosed space is,
$$\oint \textbf{E} \cdot d\textbf{a} = \frac{q}{\epsilon_0}$$
Making the charge just the flux times $\epsilon_0$. Because of the superposition principle the electric field at any point can be determined by adding together the contribution of all individual fields.
$$\textbf{E} = \sum_i^n \textbf{E}_i$$
Where, $\textbf{E} = \frac{q}{\epsilon_{0} r^{2}} = \frac{\Phi}{r^{2}}$.
If we subdivide the sphere into infinitesimally small sections we can in principle sum the various electric fields. However, since the charge is uniformly distributed, for any point within the charge there will be a $\textbf{E}$ where $r = 0$.
The electric field within a charge is therefore infinite.