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Published byGarry Parker Modified over 9 years ago
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Fraunhofer Diffraction Geometrical Optics: …light can’t turn a corner. I Bill Mageors
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Physical Optics: …actually, it can. I Francesco Maria Grimaldi Fraunhofer Diffraction
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Huygens-Fresnel Principle Every point on a wavefront may be regarded as a secondary source of spherical wavelets. The propagated wave follows the periphery of the wavelets. Huygens, just add the wavelets considering interference! Augustin-Jean Fresnel (That’s a sweet ascot by the way.)
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Far-Field Diffraction (a.k.a. Fraunhofer Diffraction) Far enough that source illumination is a plane wave. Far enough that diffracted wavelets are plane wave.
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b ds s s sin r Single Slit Fraunhofer Diffraction P
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Get the amplitudes right! field amplitude field spherical wavelets: As ds goes to zero, dE o must go to zero: field amplitude per unit width
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Get the phases right! (just like Young’s Double Slit) Integrate over the slit:
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new variable: Calculate irradiance:
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field at r an irradiance “sinc” “sampling function” “sine cardinal” Minima at: Maxima at: (graph it!)
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Beam spreading
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