Suppose $S_{1}$ and $S_{2}$ arc the slits at a distance $d$ from each other.
Distance of screen be $D$. Let $P$ be a point where there is a bright fringe.
A glass plate is placed in the path of the ray from $S_{1}$ to $P$.
We know that the path difference between the rays in absence of glass plate is $\Delta x=S_{2} P-S_{1} P=\frac{d y}{D}$
In presence of the glass plate, the optical path length of the ray from $S_{1}$ to $P$ will be different.
The total optical path length for this ray is given by
$S_{1} P-t+\mu l$
$=S_{1} P+(\mu-1) t$
Where $\mu$ is the refractive index of the glass platc and $t$ is its thickness.
Hence the new path difference is given by
$\Delta x' =S_{2} P-\left[S_{1} P+(\mu-1) t\right]$
$=\Delta x-(\mu-1) t $
$=\frac{d y}{D}-(\mu-1) t$
For a bright fringe, $\Delta x'=n \lambda$
and $y=y n=$ distance of the bright fringe from the central fringe
$\therefore \,\,\,\frac{d y_{u}}{D}-(\mu-1) t=n \lambda$
$\Rightarrow \,\,\,y_{n}=\frac{D}{d}[(\mu-1) t+n \lambda] $
$\therefore \,\,\,y_{n+1}-y_{n}=\omega=\frac{D \lambda}{d}$
Hence the fringe width remains constant.