We already know that the path difference
△x=nλ for bright fringes and
△x=(n+1/2)×λ for dark fringes
Now let us study the given figure.
Suppose S1A is the perpendiculr from S1 to S2P.
Suppose,
D=OB = seperation between slits and the screen,
d = seperation between th slits
and D>>d.
Under the above approximation S1P and S2P are nearly parallel and hence S1A is very nearly perpendicular to S1P, S2P
and OP. AS S1S2 is perpendicular to OB and S1A is perpendicular to OP, we have
∠S2S1A=∠POB=θ
This is a small angle as D>>d.
The path difference is
△x=PS2−PS1≈PS2−PA
= S2A = dsinθ≈dtanθ
= d×yD
The centers of the bright fringes are obtained atdistances y from the point B, where
△x=d×yD = nλ
or, y=nDλd i.e.,
at y = 0, ±Dλd, ±2Dλd, ±3Dλd, ....etcSimilarly we can show for dark fringes y=±Dλ2d, y=±3Dλ2d, y=±5Dλ2d,.......etc
the width fringe is therefore ,
ω=Dλd