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3. Geometrical Optics
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Geometric optics—process of light ray through lenses and mirrors to determine the location and size of the image from a given object. Reflection and Mirror
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Image Formation by Reflection
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Application of Double Reflection-Periscope
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DIY Periscope
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DIY Periscope (Cont’)
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Law of reflection (Snell’s law)
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Types of Lenses
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Ray Tracing through Thin Lenses
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Image Formation by thin Lenses Lens equation:
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ABCD Matrix
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ABCD Matrix (Cont’)
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Aberrations of Lenses Primary Aberration image deviate from the original picture/the first-order approximation Monochromatic aberrations Spherical Aberration Coma Astigmatism Curvature of field Distortion Chromatic aberration
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General Method of Reducing Aberration in Optical Systems-Multiple Lenses United States Patent 6844972
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General Method of Reducing Aberration in Optical Systems-Multiple Lenses (Cont’) United States Patent 6995908
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Chromatic Aberration The focal lengths of lights with distinct wavelengths are different.
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Solution of Chromatic Aberration-Using Doublet, Triplet, or Diffractive Lens
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Spherical Aberration (SA)
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Spherical Aberration for Different Lenses (a) Simple biconvex lens (b) “Best-form” lens (c) Two lenses (d) Aspheric, almost plano-convex lens
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Solutions of Spherical Aberration- Using Aspherical Lens or Stop
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Coma
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Coma (Cont’) (a) Negative coma (b) Postive coma
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Astigmatism
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Astigmatism (Cont’)
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Solutions of Astigmatism-Using Multiple Lenses
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Curvature of field
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Solutions of Curvature of field-Using Multiple Lenses
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Distortion Picture taken by a wide-angle camera in front of graph paper with square grids
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Solution of Distortion-Using Multiple Lenses
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Nearsightedness (Myopia) and Farsightedness (Hyperopia)
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Image Formation Camera
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Camera Eg. 50 mm camera lens, aperture stop 6.25mm: F-number = 8 (f/8) F-number Exposure E: energy collected by camera lens B: brightness of object A: area of aperture d: diameter of aperture stop
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Camera Lenses Wide-angle Lenses- the Aviogon and the Zeiss Orthometer lenses Standard Lenses-the Tessar and the Biotar lenses Lens of reducing the 3rd-order aberration- the Cooke triplet lens
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Depth of Field (DOF) The distance between the nearest and farthest objects in a scene that appear acceptably sharp in an image. In cinematography, a large DOF is called deep focus, and a small DOF is often called shallow focus. For a given F-number, increasing the magnification decreases the DOF; decreasing magnification increases DOF. For a given subject magnification, increasing the F-number increases the DOF; decreasing F-number decreases DOF.
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Numerical Aperture (NA) The numerical aperture of an optical system is a dimensionless number that characterizes the range of angles over which the system can accept or emit light. Generally, For a multi-mode optical fiber,
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Telescope
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Astronomical (Keplerian) Telescope Magnification (magnifying power): : angle subtended at input end in front of objective ’: angle subtended at output end behind eyepiece (inverted image) For small angle: General Keplerian telescope: d=f o +f e
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Galileo Telescope General Galileo telescope: d=f o -f e
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Terrestrial Telescope All images are erecting
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Optical Microscope
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Microscope Theory Objective Overall magnification: m o : linear magnification of objective m e : angular magnification of eyepiece Linear magnification: Numerical aperture (NA)
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Microscope Theory (Cont’) Angular magnification: (normal reading distance) Overall magnification of microscope: f o : focal length of objective f e : focal length of eyepiece Eyepiece
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Simple Projection System
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Fresnel Lens and Plates focusing point (in phase) Radius of the concentric circular: r n = [(n ) 2 +2fn ] ½, n=0, 1, 2,…. Sapce between two adjacent circular zone: r n = r n+1 r n
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