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Published byBasil Logan Modified over 9 years ago
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Diffraction by N-slits
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Optical disturbance due to N slits
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Contribution of j th slit
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Contribution of N slits
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Irradiance due to N-slits I 0 = I rradiance by single slit at =0
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For principal maxima or
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For minima Between consecutive principal maxima, there will be N-1 minima
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Subsidiary maxima (N-2) subsidiary maxima between consecutive principle maxima
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For large N, irradiance of first subsidiary maxima
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Diffraction from multiple slits Slit Diffraction Pattern
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Normal incidence Transmission grating
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Oblique incidence a
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For two wavelengths
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Dispersive power of grating Width of principal maxima
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Barely resolved ItIt s w
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Chromatic resolving power of a grating
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Chromatic resolving power of a prism
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Reflection grating
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Diffraction grating
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The nominal track separation on a CD is 1.6 micrometers, corresponding to about 625 tracks per millimeter. This is in the range of ordinary laboratory diffraction gratings. For red light of wavelength 600 nm, this would give a first order diffraction maximum at about 22°.
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15 15 0 nm 450 nm Atomic Force Microscope Image of CD
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Bragg’s law X-ray diffraction from crystals: 2d Sin θ = n λ
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Phase grating Delta function Bessel function
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Problem Consider a opaque screen with 5 equally spaced narrow slits (spacing between them is d) and with monochromatic plane wave (wavelength ) incident normally. Draw a sketch of the transmitted intensity vs. angle to the normal for = 0 to = 1/5 radian. Take Sin = over this range and assume d/ =10. What is the ratio of least intense to the most intense peak? What is the angular distance of the first intense peak away from = 0.
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