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Lecture 15 Ray Optics Chapter 23 PHYSICS 270 Dennis Papadopoulos March 9, 2010
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Lecture 15 Ray Optics Chapter 23 PHYSICS 270 Dennis Papadopoulos March 9, 2010.

Dec 21, 2015

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Page 1: Lecture 15 Ray Optics Chapter 23 PHYSICS 270 Dennis Papadopoulos March 9, 2010.

Lecture 15Ray Optics Chapter 23

PHYSICS 270Dennis Papadopoulos

March 9, 2010

Page 2: Lecture 15 Ray Optics Chapter 23 PHYSICS 270 Dennis Papadopoulos March 9, 2010.

θ =sin−1(λ /a)

Wave vs. Ray Model

≈ nm

Page 3: Lecture 15 Ray Optics Chapter 23 PHYSICS 270 Dennis Papadopoulos March 9, 2010.

Ray Optics

Line of sight

Self Luminous vs. Reflected

Page 4: Lecture 15 Ray Optics Chapter 23 PHYSICS 270 Dennis Papadopoulos March 9, 2010.

Important Concepts

Page 5: Lecture 15 Ray Optics Chapter 23 PHYSICS 270 Dennis Papadopoulos March 9, 2010.
Page 6: Lecture 15 Ray Optics Chapter 23 PHYSICS 270 Dennis Papadopoulos March 9, 2010.
Page 7: Lecture 15 Ray Optics Chapter 23 PHYSICS 270 Dennis Papadopoulos March 9, 2010.

Pictorial Representation - Ray Diagrams

Page 8: Lecture 15 Ray Optics Chapter 23 PHYSICS 270 Dennis Papadopoulos March 9, 2010.

Apertures – Camera Obscura

hi /ho = di /do

Page 9: Lecture 15 Ray Optics Chapter 23 PHYSICS 270 Dennis Papadopoulos March 9, 2010.

A long, thin light bulb illuminates a vertical aperture. Which pattern of light do you see on a viewing screen behind the aperture?

Page 10: Lecture 15 Ray Optics Chapter 23 PHYSICS 270 Dennis Papadopoulos March 9, 2010.

A long, thin light bulb illuminates a vertical aperture. Which pattern of light do you see on a viewing screen behind the aperture?

Light spreads horizontally due to different parts of the lightbulb

Light spreads vertically as it goes through the vertical aperture

Page 11: Lecture 15 Ray Optics Chapter 23 PHYSICS 270 Dennis Papadopoulos March 9, 2010.
Page 12: Lecture 15 Ray Optics Chapter 23 PHYSICS 270 Dennis Papadopoulos March 9, 2010.

The Plane Mirror – Virtual Image

Reflected rays coming from point P’ – The Virtual; Image Point – s=s’

Page 13: Lecture 15 Ray Optics Chapter 23 PHYSICS 270 Dennis Papadopoulos March 9, 2010.
Page 14: Lecture 15 Ray Optics Chapter 23 PHYSICS 270 Dennis Papadopoulos March 9, 2010.

Two plane mirrors form a right angle. How many images of the ball can you see in the mirrors?

A. 1

B. 2

C. 3

D. 4

Page 15: Lecture 15 Ray Optics Chapter 23 PHYSICS 270 Dennis Papadopoulos March 9, 2010.

A. 1

B. 2

C. 3

D. 4

Two plane mirrors form a right angle. How many images of the ball can you see in the mirrors?

Page 16: Lecture 15 Ray Optics Chapter 23 PHYSICS 270 Dennis Papadopoulos March 9, 2010.

Image FormationObject point (P,Q) maps to Virtual Image point (P’,Q’) : Rule

Page 17: Lecture 15 Ray Optics Chapter 23 PHYSICS 270 Dennis Papadopoulos March 9, 2010.
Page 18: Lecture 15 Ray Optics Chapter 23 PHYSICS 270 Dennis Papadopoulos March 9, 2010.

Index of Refraction

fλ = v

v = c /n

Phase of wave rotates faster in materials than in

vacuum

Page 19: Lecture 15 Ray Optics Chapter 23 PHYSICS 270 Dennis Papadopoulos March 9, 2010.

Reflection and Refraction

θi =θ r

Ptolemy 140 AD

Snell 1621sinθin sinθr

Snell’s law allow us to predict how light is going to bend in going fro air to water n=1.5

Is there a way of thinking that makes this evident and proves its generality -> Fermat

Page 20: Lecture 15 Ray Optics Chapter 23 PHYSICS 270 Dennis Papadopoulos March 9, 2010.

Fermat’s Principle of Least Time

Of all possible paths that light takes to get from one point to another light takes the path that corresponds to the shortest time

AEB=AEB’ Shortest length from A to B

after hitting the mirror is the one that goes as a straight line from A to B’, i.e. ACB’.Notice that ACB has equal incidence and reflection

angles

Angle BCF=Angle B’CF= Angle DCA

Page 21: Lecture 15 Ray Optics Chapter 23 PHYSICS 270 Dennis Papadopoulos March 9, 2010.

Fermat’s Principle for Refraction

v = c /n

v sinθ i = c sinθ rsinθ i = n sinθ r

Snell’s law

θ

θr

The slower the medium the smaller the refraction angle