# Image charges and capacitors?

Consider these two situations:

1. A (infinite) parallel plate capacitor in which one plate is held at a potential $$V$$ and the other is grounded.

2. A point charge near an infinite plane and grounded plate.

For the first situation the plates are considered to be sheet charges (this can be seen when using Gauss's law for one of the plates to determine the electric field inside the capacitor), so that we can see them as simply a layer of charges, as shown in the digram below. But in the second case we consider the plane plate to have only surface charges and no electric field inside, (this is apparent when working out the surface charge density, we take a surface that only protrudes one side of the plate). This charge distribution is shown below. In both these cases we have a near identical situation with respect to the grounded plates. So how come we get such different charge distributions, or I am mistaken in saying one is the way it is?

(Note: I am asking why the we have a 'sheet of charges' in one case but surface charges in the other rather then why we have a different spread of charges on the plates (which I think is obvious))

Edit

Let me give an example of how I would use Gauss's law and how I have seen Gauss's law applied to these two cases.

Firstly for the capacitor: Using Gauss's law on this and ignoring end effects we have $$2AE=Q/\epsilon_{0}$$ $$E=\frac{Q}{2A\epsilon_{0}}$$ But for the 'image charge' situation I would do the following: using Gauss's law: $$\delta A E=\frac{Q}{\epsilon_0}$$ $$E=\frac{Q}{\delta A \epsilon_0}$$ As can be seen these two give different values for the electric field just above the surface.