Maximum lateral displacement of a ray of light incident (i=90) on a slab of thickness t is:
We know that,
For i=900
Lateral shift is maximum
Lateral shift for a slab of t thickness
L.S=t×sin(i−r)cosr
L.S=t×sin(90−r)cosr
L.S=t×cosrcosr
L.S=t
Hence, the lateral shift is equal to thickness t