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Imaging Science FundamentalsChester F. Carlson Center for Imaging Science Mirrors and Lenses
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Imaging Science FundamentalsChester F. Carlson Center for Imaging Science Curved Mirror u Parallel light rays reflect off of a curved mirror and converge at a Focal Point u C is the Center of Curvature for the curved mirror u F is the Focal Point for incoming parallel light Axis of symmetry Light Rays F’ C
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Imaging Science FundamentalsChester F. Carlson Center for Imaging Science Review: Snell’s Law u The change in direction is described by Snell’s Law. u This change is dependent upon the index of the material (optical density) and is relative to the normal line. AIR GLASS AIR GLASS normal
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Imaging Science FundamentalsChester F. Carlson Center for Imaging Science Snell’s Law Snell’s Law: n 1 sin 1 = n 2 sin 2 11 22 n1n1 n2n2 (Or, if 1 and 2 are small, n 1 1 = n 2 2 )
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Imaging Science FundamentalsChester F. Carlson Center for Imaging Science Refraction for Different Materials AIR WATER GLASS DIAMOND light
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Imaging Science FundamentalsChester F. Carlson Center for Imaging Science Flat to Curved () Surface Flat to Curved (transmissive) Surface A curved surface can be approximated with small straight segments.
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Imaging Science FundamentalsChester F. Carlson Center for Imaging Science Graphical Ray Tracing u A way to analyze optical systems. u Modern ray tracing is often done on a computer u Light rays always travel from left to right for analysis purposes. Axis of symmetry Image side (+)Source side(-) Light Rays Lens
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Imaging Science FundamentalsChester F. Carlson Center for Imaging Science Curved Interface u Concave interface diverges rays. u Convex interface converges rays. Assuming n’ > n nn’n
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Imaging Science FundamentalsChester F. Carlson Center for Imaging Science Convex Lens shorthand In real life Double Convex Plano-Convex Positive Meniscus Types
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Imaging Science FundamentalsChester F. Carlson Center for Imaging Science Convex Lens u Image focal point, F’, is half the distance to the effective center of curvature of the lens. u Object focal point, F, is exactly the same distance on the object side of the lens. Axis of symmetry Light Rays Lens F’ F Object side Image side
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Imaging Science FundamentalsChester F. Carlson Center for Imaging Science Convex Lens u Image focal length, f’, is the distance from the lens to the image focal point. u Object focal length, f, is the distance from the lens to the object focal point. F’ f’ F f
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Imaging Science FundamentalsChester F. Carlson Center for Imaging Science Ray Diagrams for a Positive (Convex) Lens (infinity) Object Location Image Type and Location Real, at F’ F Real, at 2F’ Real, at (infinity) Virtual 2F < F
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Imaging Science FundamentalsChester F. Carlson Center for Imaging Science Real vs. Virtual Images u Real Image: Image formed where light rays actually converge and pass through a specific point. Real images can be projected onto paper or a screen. u Virtual Image: Image formed where light rays appear to diverge from. Virtual images cannot be projected onto paper or a screen.
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Imaging Science FundamentalsChester F. Carlson Center for Imaging Science Concave Lens shorthand In real life Double concave Plano- concave Negative meniscus Types
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Imaging Science FundamentalsChester F. Carlson Center for Imaging Science Concave Lens u Image focal point, F’, is on the object side u Focal length, f’, is negative. Axis of symmetry Light Rays Lens F’ f’
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Imaging Science FundamentalsChester F. Carlson Center for Imaging Science Ray Diagrams for a Negative (Concave) Lens Rays converging toward F Object Location Image Type and Location Virtual, at (infinity) Approaching the lens from (infinity) Virtual, at F’ Virtual, between F’ and the lens (infinity)
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Imaging Science FundamentalsChester F. Carlson Center for Imaging Science Aberrations u Spherical lenses and mirrors, even if ground and polished perfectly, do not produce perfect images. u The deviation in the image is called an aberration.
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Imaging Science FundamentalsChester F. Carlson Center for Imaging Science Chromatic Aberration u Dispersion results in a lens having different focal points for different wavelengths - this effect is called chromatic aberration. u Results in a “halo” of colors. u Solution: Use 2 lenses of different shape and material (“achromatic doublet”). F’ Red. Object (small dot)Image with chromatic aberration F’ Blue White light
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Imaging Science FundamentalsChester F. Carlson Center for Imaging Science Spherical Aberration u All the rays do not bend toward the focal point, resulting in a blurred spot. u Solution: use lenses with aspherical curvature, or use a compound lens. F’. Object (small dot)Image with spherical aberration
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Imaging Science FundamentalsChester F. Carlson Center for Imaging Science Other Aberrations u Coma u Off axis blur which looks like the “coma” of a comet. u Astigmatism u Different focal lengths for different planes. u Distortion u Images formed out of shape...
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