Split Lens Modification
Meslin modified the Billet split lens to produced circular fringes. The two portions of the Billet split lens L1 and L2 are made coplanar and the lower portion L2 is displaced through a distance y. A monochromatic source S is used and light passing through L1 forms an image of the source at A and that passing through L2 forms an image of the source at B. The two sources A and B are coherent and the fringes are produced on a screen normal to A and B. The screen is situated between A and B.
Consider any point P in the interference field. The light reaching P from S through L1 transverses an optical path d1 + AP, where d1 is the optical path from S to A. Moreover, d1 is constant because S and A are conjugate points. Similarly, light reaching P from S through L2 transverses an optical path = d2 – BP, where d2 is optical path from S to B.
Here d2 is constant because S and B are conjugate points. Therefore, the path difference between the rays reaching P is given by
x = (d2 – BP) – (d1 + AP)
x = (d2 – d1) – (BP + AP)
But, d2 – d1 is constant.
Therefore, for x to be constant, (BP + AP) should be constant. Thus, the locus of the points for which the optical path difference (x) should be constant, will be an ellipsoid of revolution having A and B as foci. The cross-section of this surface by a plane normal to AB will be a circle. Hence, alternatively bright and dark circular fringes will be formed on the screen. Here, the beams interfere only on one side. Therefore semicircular fringes will be produced on the screen.
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