Suppose I have two parallel plates, positively and uniformly charged, a distance $d$ apart and infinite. The surface charge density of the top plate is $\sigma_1$ and the surface charge density of the bottom plate is $\sigma_2$. Then the electric field inside of the plates can be given by (I used Gauss' Law to show this easily): $$\vec{E} = \vec{E_{\text{top}}} + \vec{E_{\text{bottom}}} = - \frac{\sigma_1}{2\varepsilon_0}\hat{z} + \frac{\sigma_2}{2\varepsilon_0}\hat{z} = \frac{\sigma_2 - \sigma_1}{2\varepsilon_0}\hat{z}$$ The issue I'm having here is that because these two plates are both positively charged, I'm sure they need to repel. However, if $\sigma_1 > \sigma_2$, the electric field inside the plates points downwards, which suggests that the upper plate moves towards the lower plate? Isn't that suggesting they're attractive.
As you can see, I'm having a bit of difficulty understanding what this result about the electric field is telling us for how the plates would move in the different cases that arise for $\sigma_1$ and $\sigma_2$, so any help on that would be appreciated.