Consider the arrangement shown in figure (17-E7). By some mechanism, the separation between the slits S3 and S4 can be changed. The intensity is measured at the point P which is at the common perpendicular bisector of S1S2 and S3S4. When
, the intensity measured at P is I. Find this intensity when z is equal to

Let the intensity of slits
and
be
. For
and
, The distance from the central maximum is
.
So the path difference is ![]()
Given, ![]()
![]()
And the corresponding phase difference is
![]()
Now, intensity at each slit is given by
![]()
Here, P is also central maxima. So the intensity is![]()
![]()
(a)For
,
and ![]()
![]()
Therefore, intensity at each slit is
.
This means that both slits
and
would be dark. Thus intensity at P would be zero.
(b)For
,
and ![]()
![]()
Therefore, intensity at each slit is
.
Hence intensity at P is ![]()
(c)For
,
and ![]()
![]()
Therefore, intensity at each slit is
.
Hence intensity at P is ![]()
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