*16 Babinet's principle. A monochromatic beam of paral- lel light is incident on a "colli- mating" hole of diameter x> A. Point P lies in the geometrical shadow region on a distant screen (Fig. 36-39a). Two dif- fracting objects, shown in Fig. 36-39b, are placed in turn over the collimating hole. Object A is an opaque circle with a hole in it, and B is the "photographic negative" of A. Using superpo- sition concepts, show that the intensity at P is identical for the two diffracting objects A and B. Screen (a) (6)

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*16 Babinet's principle. A
monochromatic beam of paral-
lel light is incident on a "colli-
mating" hole of diameter x> A.
Point P lies in the geometrical
shadow region on a distant
screen (Fig. 36-39a). Two dif-
fracting objects, shown in Fig.
36-39b, are placed in turn over
the collimating hole. Object A is
an opaque circle with a hole in
it, and B is the "photographic
negative" of A. Using superpo-
sition concepts, show that the
intensity at P is identical for the
two diffracting objects A and B.
Screen
(a)
(6)
Transcribed Image Text:*16 Babinet's principle. A monochromatic beam of paral- lel light is incident on a "colli- mating" hole of diameter x> A. Point P lies in the geometrical shadow region on a distant screen (Fig. 36-39a). Two dif- fracting objects, shown in Fig. 36-39b, are placed in turn over the collimating hole. Object A is an opaque circle with a hole in it, and B is the "photographic negative" of A. Using superpo- sition concepts, show that the intensity at P is identical for the two diffracting objects A and B. Screen (a) (6)
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