The solution of $$\frac{\partial c}{\partial t} = D\frac{\partial^2c}{\partial x^2}$$ with boundary conditions $$\begin{cases} c(x,0) = C^\infty\\ c(0,t)=0\\ c(\infty,t)=C^\infty \end{cases}$$ is $$c(x,t) = C^\infty \operatorname{erfc}\Big(\frac{x}{2\sqrt{Dt}}\Big)$$ and then the flux is, $$J_{(x=0)} = D\frac{\partial c(x,t)}{\partial t} = \frac{C^\infty\sqrt{D}}{\sqrt{\pi t}}$$ what is the limit (maximum) of $J$?
When $t \to 0$ (at short times) then $J \to \infty$. It doesn't make sense.