A point object O is placed in front of a transparent slab at a distance x from its closer surface. It is seen from the other side of the slab by light incident nearly normally to the slab. The thickness of the slab is t and its refractive index is μ. The apparent shift in the position of the object is
t(1−tμ)
The situation is shown in figure. Because of the refraction at the first surface, the image of O is formed at O1. For this refractiion, the real depth is AO = x and the apparent depth is AO1. Also the first medium is air and the second is the slab. Thus,
xAO1=1μor,AO1=μx.
The point O1 acts as the object for the refractiion at the second surface. Due to this refraction the image of O1 is formed at I. Thus,
BO1BI=μ
or, AB+AO1BI=μ or t+μxBI=μ
or BI=x+tμ.
The net shift in OI=OB−BI=(x+t)−(x+tμ)
=t(1−tμ)
which is independent of x.