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Two coherent point light sources of same frequency are placed at x = -d/2 and x = d/2. These source are surrounded by a spherical screen having equationx 2 + y 2 + z 2 = R 2 (where R ≫ d) . The sources emit monochromatic light of wavelength (λ =d/3). Waves from both the sources reach screen and superimpose. When waves reaching any point on the screen have a constant path difference of nλ (where λ is wavelength of light and ‘n’ is some integer), the superposition of these waves is constructivein nature (i.e. maximum intensity) n may be called as order of maximum.
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Two coherent point light sources of same frequency are placed at x = -d/2 and x = d/2. These source are surrounded by a spherical screen having equation
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