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3. Geometrical Optics. Geometric optics—process of light ray through lenses and mirrors to determine the location and size of the image from a given object.

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Presentation on theme: "3. Geometrical Optics. Geometric optics—process of light ray through lenses and mirrors to determine the location and size of the image from a given object."— Presentation transcript:

1 3. Geometrical Optics

2 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

3 Image Formation by Reflection

4 Application of Double Reflection-Periscope

5 DIY Periscope

6 DIY Periscope (Cont’)

7 Law of reflection (Snell’s law)

8 Types of Lenses

9 Ray Tracing through Thin Lenses

10 Image Formation by thin Lenses Lens equation:

11 ABCD Matrix

12 ABCD Matrix (Cont’)

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20 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

21 General Method of Reducing Aberration in Optical Systems-Multiple Lenses United States Patent 6844972

22 General Method of Reducing Aberration in Optical Systems-Multiple Lenses (Cont’) United States Patent 6995908

23 Chromatic Aberration The focal lengths of lights with distinct wavelengths are different.

24 Solution of Chromatic Aberration-Using Doublet, Triplet, or Diffractive Lens

25 Spherical Aberration (SA)

26 Spherical Aberration for Different Lenses (a) Simple biconvex lens (b) “Best-form” lens (c) Two lenses (d) Aspheric, almost plano-convex lens

27 Solutions of Spherical Aberration- Using Aspherical Lens or Stop

28 Coma

29 Coma (Cont’) (a) Negative coma (b) Postive coma

30 Astigmatism

31 Astigmatism (Cont’)

32 Solutions of Astigmatism-Using Multiple Lenses

33 Curvature of field

34 Solutions of Curvature of field-Using Multiple Lenses

35 Distortion Picture taken by a wide-angle camera in front of graph paper with square grids

36 Solution of Distortion-Using Multiple Lenses

37 Nearsightedness (Myopia) and Farsightedness (Hyperopia)

38 Image Formation  Camera

39 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

40 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

41 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.

42 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,

43 Telescope

44 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

45 Galileo Telescope General Galileo telescope: d=f o -f e

46 Terrestrial Telescope All images are erecting

47 Optical Microscope

48 Microscope Theory Objective Overall magnification: m o : linear magnification of objective m e : angular magnification of eyepiece Linear magnification: Numerical aperture (NA)

49 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

50 Simple Projection System

51 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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