∠i=∠e<∠r
∠i<∠e<∠r
∠i>∠e>∠r
∠i=∠e>∠r
As the incident ray is parallel to the emergent ray, thus the incidence angle is equal to the emergence angle i.e., ∠i=∠e. Also, the ray traveling from a rarer medium (air) to a denser medium (glass slab) slightly bends towards the normal after refraction, thus the angle of refraction is smaller than the angle of incidence i.e., ∠r<∠i ⇒ ∠i=∠e>∠r