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Physics 1230: Light and Color Ivan I. Smalyukh, Instructor

Office: Gamow Tower, F-521 Email: ivan.smalyukh@colorado.edu Phone: 303-492-7277 Lectures: Tuesdays & Thursdays, 3:30 PM - 4:45 PM Office hours: Mondays & Fridays, 3:30 PM – 4:30 PM TA: Jhih-An Yang jhihan.yang@colorado.edu.

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Physics 1230: Light and Color Ivan I. Smalyukh, Instructor

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  1. Office: Gamow Tower, F-521 • Email: • ivan.smalyukh@colorado.edu • Phone: 303-492-7277 • Lectures: • Tuesdays & Thursdays, • 3:30 PM - 4:45 PM • Office hours: • Mondays & Fridays, • 3:30 PM – 4:30 PM • TA: Jhih-An Yang • jhihan.yang@colorado.edu Physics 1230: LightandColorIvan I. Smalyukh, Instructor Class # 11

  2. Announcements • HW #3 Due Sept 29; • Exam #1 - October 11; • Overview of Exam #1 material – Sept 29;

  3. Note light-focusing property of convex (converging) lens a good light collector or solar oven; can also fry ants with sunlight, but please don’t do that unless you’re going to eat them

  4. Note light-dispersing property of convex lens The “backwards” light collector: create a collimated light beam

  5. Thin convex lens: three easy rules for ray tracing } focal length • A ray parallel to the axis is deflected through the focus on the other side • A ray through the center of the lens continues undeviated • A ray coming from the focus on one side goes out parallel to the axis on the other 1 2 F’ F 3 3 foci Ray might have to be extended

  6. Where will this ray go? Ray Tracing foci (focuses?)

  7. Ray Tracing Where will this ray go? Suppose it’s emitted from this object foci (focuses?)

  8. Ray Tracing Where will this ray go? Suppose it’s emitted from this object We know where these 3 rays go, using the simple ray rules foci (focuses?)

  9. Ray Tracing Amazing property of this lens: all rays from the object will converge to the same point Where will this ray go? Suppose it’s emitted from this object We know where these 3 rays go, using the simple ray rules foci (focuses?)

  10. Ray Tracing Amazing property of this lens: all rays from the object will converge to the same point Where will this ray go? Suppose it’s emitted from this object We know where these 3 rays go, using the simple ray rules foci (focuses?)

  11. Ray Tracing: thin lens, object outside focus See how the rays emerge from this point (the image)? Amazing property of this lens: all rays from the object will converge to the same point (the image)

  12. Ray Tracing: thin lens, object outside focus Amazing property of this lens: all rays from the object will converge to the same point (the image) Eye sees an image here. The Lens acts as our “Magic Ray Machine”, creating the rays to produce an image.

  13. A Question In this case, the image is: • Virtual • Real Real because the light rays really go through the image. You can put a screen there to see it. Eye sees an image here.

  14. Two point sources of light are imaged onto a screen by a converging lens. The images are labeled 1 and 2. You slide a mask over the left half of the lens. What happens to the images? A Question • Image 1 vanishes • Image 2 vanishes • Something else happens

  15. Two point sources of light are imaged onto a screen by a converging lens. The images are labeled 1 and 2. You slide a mask over the left half of the lens. What happens to the images? A Question • Image 1 vanishes • Image 2 vanishes • Something else happens The image gets dimmer, but half the lens is still a lens, and it produces a pair of images.

  16. Thin concave (diverging) lens Guess how this ray will be bent: F’ F For diverging lens focal length defined to be negative (of the distance between focus and lens)

  17. Thin concave (diverging) lens F’ F For diverging lens focal length defined to be negative

  18. Thin concave (diverging) lens: three easy ray rules • A ray parallel to the axis is deflected as if it came from the focus • A ray through the center of the lens continues undeviated • A ray aimed at the focus on the other side comes out parallel 1 2 F’ F 3 Ray might have to be extended For diverging lens focal length defined to be negative

  19. 1 1 F’ F’ F F Difference between convex (converging) & concave (diverging) lenses (Rule 3, the backwards version of rule 1, also differs)

  20. Ray tracing a convex lens: object inside focus

  21. Ray tracing a convex lens: object inside focus The image appears larger (and farther away) than the object. This is a magnifying glass. (Remember: a magnifying glass is a convex lens.) Aside: near-sighted people need concave/diverging lenses; can a marooned myopic start a fire with his eye-glasses?

  22. Convex lens ray tracing: 3 cases Like concave mirrors, convex lenses have 3 kinds of cases for ray tracing: 1. object inside focal length 2. object outside focal length, inside twice focal length 3. object outside twice focal length You can do the ray tracing and answer the following questions: Is the image real/virtual? Is the image larger/smaller than the object? Is the image erect/inverted? How can the lens be used?

  23. Ch. 3 – Spherical mirrors and lenses Virtual images (review) Spherical mirrors Spherical lenses Thin lens approximation Formulas Magnification Adding lenses Image distance 4. Aberrations of lenses We are here 23 23

  24. Object distance, image distance, focal length Xo Xi F

  25. Magnification formula S0 = object height Si = image height Note the similar triangles. Distances below the horizontal axis are defined as negative. Demo: big mama lens and bulb

  26. Image distance equation F = focal length XO = object distance XI = image distance Usually, F is given. Distant objects: Let Xo be very large, say 1,000,000 meters. Then 1/Xo = 0.000001, which is very small. You can ignore it. Then For distant objects, the image is at the focal point (ask a burnt ant) Demo: find focal length of lenses

  27. What is lens power (or diopters)? Lens power: D = 1/F Units of D are 1/meters, also called diopters Eyeglass lenses are measured in diopters. Example: D = 2/m = what focal length? F = 1/D = 1/(2/m) = (1/2) m = 0.5 m

  28. How thin lenses add Ftot = final focal length F1= focal length lens 1 F2 = focal length lens 2 Diverging lenses (concave) have negative focal lengths This is the same as adding powers: Dtot = D1 + D2 Demo: put together some lenses

  29. Compound Lenses • Can have less aberration. • A modern lens can have 16 elements and can “zoom”. “stop” Reduces aberration Image plane

  30. Ch. 3 – Spherical mirrors and lenses Virtual images (review) Spherical mirrors Spherical lenses 3 formulas Aberrations of lenses We are here 30 30

  31. Aberrations • Field curvature • Off-axis aberration • Spherical aberration • Distortion • Chromatic aberration

  32. Aberration: field curvature Image does not lie in one plane

  33. Off axis aberration Edges of images are less clear. Demo with lens and bulb

  34. Spherical aberration Rays at the edge focus closer to the mirror Demo with lens, not mirror

  35. Aberrations: Distortion Demo with overhead and small lenses

  36. Chromatic Aberration Demo with lens and bulb

  37. Web tutorials with Java Applets • Useful web links on curved mirrors • http://micro.magnet.fsu.edu/primer/java/mirrors/concavemirrors/index.html • http://micro.magnet.fsu.edu/primer/java/mirrors/convexmirrors/index.html • http://micro.magnet.fsu.edu/primer/java/mirrors/concave.html • Useful web links on lenses • http://micro.magnet.fsu.edu/primer/lightandcolor/lenseshome.html • http://micro.magnet.fsu.edu/primer/java/lenses/simplethinlens/index.html • http://micro.magnet.fsu.edu/primer/java/lenses/converginglenses/index.html • http://micro.magnet.fsu.edu/primer/java/lenses/diverginglenses/index.html • http://micro.magnet.fsu.edu/primer/java/components/perfectlens/index.html • http://micro.magnet.fsu.edu/primer/java/mirrors/convex.html 37

  38. Fresnel Lens Used in lighthouses Lighthouse lens Fresnel stage light

  39. http://sandiartfullyyours.com/NewFiles/lighthouse3/images/Ponce%20Fresnell.jpghttp://sandiartfullyyours.com/NewFiles/lighthouse3/images/Ponce%20Fresnell.jpg

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