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Coherent Sources
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Wavefront splitting Interferometer
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Young’s Double Slit Experiment
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Young’s double slit © SPK
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Path difference:
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For a bright fringe, For a dark fringe, m: any integer
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For two beams of equal irradiance (I 0 )
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Visibility of the fringes (V) Maximum and adjacent minimum of the fringe system
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Photograph of real fringe pattern for Young’s double slit
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The two waves travel the same distance –Therefore, they arrive in phase S S'S'
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The upper wave travels one wavelength farther –Therefore, the waves arrive in phase S S'S'
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The upper wave travels one-half of a wavelength farther than the lower wave. This is destructive interference S S'S'
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Young’s Double Slit Experiment provides a method for measuring wavelength of the light This experiment gave the wave model of light a great deal of credibility. Uses for Young’s Double Slit Experiment
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Wavefront splitting interferometers Young’s double slit Fresnel double mirror Fresnel double prism Lloyd’s mirror
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Confocal hyperboloids of revolution in 3D S S Path difference -confocal hyperbolae with S and S as common foci =m
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Transverse section –Straight fringes S S d P D O x
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The distance of m th bright fringe from central maxima Fringe separation/ Fringe width
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Longitudinal section –Circular fringes P O rnrn S S d D N
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Path difference = d For central bright fringe
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Radius of nth bright ring For small m
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Wavefront splitting interferometers Young’s double slit Fresnel double mirror Fresnel double prism Lloyd’s mirror
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Interference fringes Real Virtual Localized Non-localized
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Localized fringe Observed over particular surface Result of extended source
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Non-localized fringe Exists everywhere Result of point/line source
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Concordance
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Discordance = (q+1/2)
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Division of Amplitude
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Phase Changes Due To Reflection An electromagnetic wave undergoes a phase change of 180° upon reflection from a medium of higher index of refraction than the one in which it was traveling –Analogous to a reflected pulse on a string μ1 μ1 μ2 μ2
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Phase shift
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D nfnfnfnf n1n1n1n1 n2n2n2n2 B d A C tttt iiii tttt tttt A B C D
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Optical path difference for the first two reflected beams
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Condition for maxima Condition for minima
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Fringes of equal thickness Constant height contour of a topographial map
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Wedge between two plates 1 2 glass glass air D t x Path difference = 2t Phase difference = 2kt - (phase change for 2, but not for 1) Maxima 2t = (m + ½) o /n Minima 2t = m o /n
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Newton’s Ring Ray 1 undergoes a phase change of 180 on reflection, whereas ray 2 undergoes no phase change R= radius of curvature of lens r=radius of Newton’s ring
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Reflected Newton’s Ring
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Newton’s Ring
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1. Optics Author: Eugene Hecht Class no. 535 HEC/O Central library IIT KGP
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