(a) For the surface charge density of a single plate.
Let the surface charge density at both sides be σ1 & σ2


(b) Electric field to the left of the plates = σ/ ε0

Since σ = Q/2A
Hence Electricfield = Q/2Aε0
This must be directed toward left as ‘X’ is the charged plate.
(c) & (d) Here in both the cases the charged plate ‘X’ acts as the only source of electric field, with (+ve) in the inner side and ‘Y’ attracts towards it with (-ve) he in its inner side. So for the middle portion E = Q/2Aε0 towards right.
(d) Similarly for extreme right the outerside of the ‘Y’ plate acts as positive and hence it repels to the right with E = Q/2Aε0