In the ideal double-slit experiment, when a glass plate (refractive index 1.5) of thickness t is introduced in the path of one of the interfering beams (wavelength λ ), the intensity at the position where the central maximum occurred previously remains unchanged. The minimum thickness of the glass plate is:
Δy=D(μ−1)td --(1)
Δy=λDd−−−−(2) (For having some intensity at central
maximum)
From 1 and 2
λDd=D(μ−1)td
λ=(1.5−1)t
t=λ1.5−1
=λ0.5
=2λ.