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Snell’s Law, Total Internal Reflection, Brewster’s Angle, Dispersion, Lenses   Physics 102:   Lecture 18
Summary of today’s lecture ,[object Object],[object Object],[object Object],[object Object],[object Object]
Demo: Snell’s Law n 2 n 1   > n 2   When light travels from one medium to another the speed changes  v=c/n, but the frequency is constant.  So the light bends: n 1  sin(  1 )= n 2  sin(  2 )   n 1  > n 2       2  >   1   Light bent  away  from normal as it goes in medium with  lower  n  1  2  r incident reflected refracted
1) Total Internal Reflection normal n 2 n 1  > n 2 Snell’s Law:  n 1  sin(  1 )= n 2  sin(  2 ) (n 1  > n 2       2  >   1  )  1  = sin -1 (n 2 /n 1 )  then   2  = 90 Light incident at a larger angle will only have reflection (  i  =   r ) For water/air: n 1 =1.33, n 2 =1  1  = sin -1 (n 2 /n 1 ) = 48.8 0 “ critical angle”  1  2  i  >   c  r  c
Fiber Optics Telecommunications Arthoscopy Laser surgery Total Internal Reflection only works if n outside  < n inside   At each contact w/ the glass air interface, if the light hits at greater than the critical angle, it undergoes total internal reflection and stays in the fiber. n inside n outside
Can the person standing on the edge of the pool be prevented from seeing the light by  total internal reflection ? 1)  Yes 2) No Preflight 18.1
ACT: Refraction ,[object Object],[object Object]
2) Brewster’s angle When angle between  reflected  beam and  refracted  beam is exactly 90 degrees, reflected beam is 100% horizontally polarized ! Reflected light is usually unpolarized (mixture of horizontally and vertically polarized).  But… n 1  sin   B  = n 2  sin (90-  B )  n 1  sin   B  = n 2  cos (  B )  horiz. and vert. polarized  B  B 90º –   B 90º horiz. polarized only! n 1 n 2
ACT: Brewster’s Angle When a polarizer is placed between the light source and the surface with transmission axis aligned as shown, the intensity of the reflected light: (1) Increases (2) Unchanged (3) Decreases T.A.
Preflight 18.3, 18.4 ,[object Object],[object Object],[object Object],[object Object],Polarizing sunglasses are often considered to be better than tinted glasses because they… Polarizing sunglasses (when worn by someone standing up) work by  absorbing  light polarized in which direction? ,[object Object],[object Object]
3) Dispersion Prism Blue light gets deflected more n blue  >  n red The index of refraction  n  depends on color! In glass:  n blue  = 1.53 n red  = 1.52 White light  blue  <   red  red  i  blue
Skier sees  blue coming up from the bottom (1) , and  red coming down from the top (2)  of the rainbow. Rainbow:  Preflight 18.5 Wow look at the variation in index of refraction! Which is  red ? Which is  blue ? Blue light is deflected more!
LIKE SO! In second rainbow pattern is reversed
4) Lenses Focal point determined by  geometry  and  Snell’s Law : n 1  sin(  1 ) = n 2  sin(  2 ) Converging lens: –  Rays parallel to P.A. converge on focal point  Diverging lens: –  Rays parallel to P.A. diverge as if emerging from focal point behind lens Larger n 2 /n 1  = more bending, shorter focal length. Smaller n 2 /n 1  = less bending, longer focal length. n 1  = n 2   => No Bending, f = infinity F         “ Plano-convex” “ Plano-concave” P.A. F P.A.
Converging & Diverging Lenses Converging lens: –  Rays parallel to P.A. converge on focal point  Diverging lens: –  Rays parallel to P.A. diverge as if emerging from focal point behind lens “ Plano-convex” “ Plano-concave” Converging = fat in the middle Diverging = thin in the middle “ Double concave” “ Double convex” = = = = “ Convex-concave” “ Concave-convex”
1)  Rays  parallel  to principal axis pass through focal point. 2)  Rays through  center  of lens are not refracted. 3)  Rays  through F  emerge parallel to principal axis. Converging Lens Principal Rays F F Object P.A. Image is:  real, inverted  and  enlarged  (in this case). Example Image Key assumptions:   •  monochromatic light incident on a  thin  lens. •  rays are all “near” the principal axis.
Converging Lens All rays parallel to principal axis pass through focal point F. Double Convex P.A. n lens  > n outside F ,[object Object],[object Object],[object Object],P.A. F Preflight 18.6 A beacon in a lighthouse produces a parallel beam of light.  The beacon consists of a bulb and a converging lens.  Where should the bulb be placed?
3 Cases for Converging Lenses This could be used in a camera.  Big object on small film Inverted Reduced Real Past 2F This could be used as a projector. Small slide on big screen Inverted Enlarged Real Between F & 2F This is a magnifying glass Upright Enlarged Virtual Inside F Object Image Image Object Image Object
ACT: Converging Lens ,[object Object],[object Object],[object Object],[object Object],F F Object P.A.
1)  Rays  parallel  to principal axis pass through focal point. 2)  Rays through  center  of lens are not refracted. 3)  Rays  toward F  emerge parallel to principal axis. Diverging Lens Principal Rays F F Object P.A. Only 1 case for diverging lens : Image is always  virtual, upright, and reduced . Example Image
[object Object],[object Object],[object Object],[object Object],ACT: Diverging Lenses Demo F F Object P.A.

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Lect18 handout

  • 1. Snell’s Law, Total Internal Reflection, Brewster’s Angle, Dispersion, Lenses Physics 102: Lecture 18
  • 2.
  • 3. Demo: Snell’s Law n 2 n 1 > n 2 When light travels from one medium to another the speed changes v=c/n, but the frequency is constant. So the light bends: n 1 sin(  1 )= n 2 sin(  2 ) n 1 > n 2   2 >  1 Light bent away from normal as it goes in medium with lower n  1  2  r incident reflected refracted
  • 4. 1) Total Internal Reflection normal n 2 n 1 > n 2 Snell’s Law: n 1 sin(  1 )= n 2 sin(  2 ) (n 1 > n 2   2 >  1 )  1 = sin -1 (n 2 /n 1 ) then  2 = 90 Light incident at a larger angle will only have reflection (  i =  r ) For water/air: n 1 =1.33, n 2 =1  1 = sin -1 (n 2 /n 1 ) = 48.8 0 “ critical angle”  1  2  i >  c  r  c
  • 5. Fiber Optics Telecommunications Arthoscopy Laser surgery Total Internal Reflection only works if n outside < n inside At each contact w/ the glass air interface, if the light hits at greater than the critical angle, it undergoes total internal reflection and stays in the fiber. n inside n outside
  • 6. Can the person standing on the edge of the pool be prevented from seeing the light by total internal reflection ? 1) Yes 2) No Preflight 18.1
  • 7.
  • 8. 2) Brewster’s angle When angle between reflected beam and refracted beam is exactly 90 degrees, reflected beam is 100% horizontally polarized ! Reflected light is usually unpolarized (mixture of horizontally and vertically polarized). But… n 1 sin  B = n 2 sin (90-  B ) n 1 sin  B = n 2 cos (  B ) horiz. and vert. polarized  B  B 90º –  B 90º horiz. polarized only! n 1 n 2
  • 9. ACT: Brewster’s Angle When a polarizer is placed between the light source and the surface with transmission axis aligned as shown, the intensity of the reflected light: (1) Increases (2) Unchanged (3) Decreases T.A.
  • 10.
  • 11. 3) Dispersion Prism Blue light gets deflected more n blue > n red The index of refraction n depends on color! In glass: n blue = 1.53 n red = 1.52 White light  blue <  red  red  i  blue
  • 12. Skier sees blue coming up from the bottom (1) , and red coming down from the top (2) of the rainbow. Rainbow: Preflight 18.5 Wow look at the variation in index of refraction! Which is red ? Which is blue ? Blue light is deflected more!
  • 13. LIKE SO! In second rainbow pattern is reversed
  • 14. 4) Lenses Focal point determined by geometry and Snell’s Law : n 1 sin(  1 ) = n 2 sin(  2 ) Converging lens: – Rays parallel to P.A. converge on focal point Diverging lens: – Rays parallel to P.A. diverge as if emerging from focal point behind lens Larger n 2 /n 1 = more bending, shorter focal length. Smaller n 2 /n 1 = less bending, longer focal length. n 1 = n 2 => No Bending, f = infinity F         “ Plano-convex” “ Plano-concave” P.A. F P.A.
  • 15. Converging & Diverging Lenses Converging lens: – Rays parallel to P.A. converge on focal point Diverging lens: – Rays parallel to P.A. diverge as if emerging from focal point behind lens “ Plano-convex” “ Plano-concave” Converging = fat in the middle Diverging = thin in the middle “ Double concave” “ Double convex” = = = = “ Convex-concave” “ Concave-convex”
  • 16. 1) Rays parallel to principal axis pass through focal point. 2) Rays through center of lens are not refracted. 3) Rays through F emerge parallel to principal axis. Converging Lens Principal Rays F F Object P.A. Image is: real, inverted and enlarged (in this case). Example Image Key assumptions: • monochromatic light incident on a thin lens. • rays are all “near” the principal axis.
  • 17.
  • 18. 3 Cases for Converging Lenses This could be used in a camera. Big object on small film Inverted Reduced Real Past 2F This could be used as a projector. Small slide on big screen Inverted Enlarged Real Between F & 2F This is a magnifying glass Upright Enlarged Virtual Inside F Object Image Image Object Image Object
  • 19.
  • 20. 1) Rays parallel to principal axis pass through focal point. 2) Rays through center of lens are not refracted. 3) Rays toward F emerge parallel to principal axis. Diverging Lens Principal Rays F F Object P.A. Only 1 case for diverging lens : Image is always virtual, upright, and reduced . Example Image
  • 21.

Editor's Notes

  1. 1
  2. Demo 281: Snell’s Law
  3. Demo 281: Snell’s Law Only possible if n1&gt;n2
  4. ACT, then demo 1129 (ball in tub of water)
  5. ACT, then demo 664
  6. refraction, reflection, refraction
  7. Start this by :35 Lens in water has larger focal length since n 2 /n 1 is smaller!
  8. Start this by :35 Lens in water has larger focal length since n 2 /n 1 is smaller!
  9. Demo 71
  10. Demo 71