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Lecture 17 Ray Optics-3 Chapter 23 PHYSICS 270 Dennis Papadopoulos March 22, 2010.

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Lecture 17 Ray Optics-3 Chapter 23 PHYSICS 270 Dennis Papadopoulos March 22, 2010
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Page 1: Lecture 17 Ray Optics-3 Chapter 23 PHYSICS 270 Dennis Papadopoulos March 22, 2010.

Lecture 17Ray Optics-3 Chapter 23

PHYSICS 270Dennis Papadopoulos

March 22, 2010

Page 2: Lecture 17 Ray Optics-3 Chapter 23 PHYSICS 270 Dennis Papadopoulos March 22, 2010.
Page 3: Lecture 17 Ray Optics-3 Chapter 23 PHYSICS 270 Dennis Papadopoulos March 22, 2010.

Total Internal Reflection

Page 4: Lecture 17 Ray Optics-3 Chapter 23 PHYSICS 270 Dennis Papadopoulos March 22, 2010.
Page 5: Lecture 17 Ray Optics-3 Chapter 23 PHYSICS 270 Dennis Papadopoulos March 22, 2010.

Image by Refraction

1 1 2

2 2 1

1 2

tan sin

tan sin

, 1

s s s s

for

l = stanθ1 = s' tanθ2

Page 6: Lecture 17 Ray Optics-3 Chapter 23 PHYSICS 270 Dennis Papadopoulos March 22, 2010.

EXAMPLE 23.13 A goldfish in a bowl

Page 7: Lecture 17 Ray Optics-3 Chapter 23 PHYSICS 270 Dennis Papadopoulos March 22, 2010.

What is a lens?Device that provides a capability to create bright and well focused images. How?

Use Refraction to create images out of divergent light rays

• Focal point

• Focal length

• Property of lens no matter how it is used

• Distance from lens that paraxial rays converge

• Reversibility

Page 8: Lecture 17 Ray Optics-3 Chapter 23 PHYSICS 270 Dennis Papadopoulos March 22, 2010.

Converging and Diverging Lenses

Page 9: Lecture 17 Ray Optics-3 Chapter 23 PHYSICS 270 Dennis Papadopoulos March 22, 2010.

Thin Lenses – Real Image –Special Rays

Thin lens-> d<<f,s,s’

1

s+

1

s'=

1

f Inverted Image

Page 10: Lecture 17 Ray Optics-3 Chapter 23 PHYSICS 270 Dennis Papadopoulos March 22, 2010.

Thin Lenses: Ray Tracing

Page 11: Lecture 17 Ray Optics-3 Chapter 23 PHYSICS 270 Dennis Papadopoulos March 22, 2010.

Tactics: Ray tracing for a converging lens

Page 12: Lecture 17 Ray Optics-3 Chapter 23 PHYSICS 270 Dennis Papadopoulos March 22, 2010.

Tactics: Ray tracing for a converging lens

Page 13: Lecture 17 Ray Optics-3 Chapter 23 PHYSICS 270 Dennis Papadopoulos March 22, 2010.

Lateral MagnificationThe image can be either larger or smaller than the object, depending on the location and focal length of the lens. The lateral magnification m is defined as

1. A positive value of m indicates that the image is upright relative to the object. A negative value of m indicates that the image is inverted relative to the object.

2. The absolute value of m gives the size ratio of the image and object: h'/h = |m| .

Page 14: Lecture 17 Ray Optics-3 Chapter 23 PHYSICS 270 Dennis Papadopoulos March 22, 2010.

s>f h’/h=s’/s

Page 15: Lecture 17 Ray Optics-3 Chapter 23 PHYSICS 270 Dennis Papadopoulos March 22, 2010.

Virtual Image

s’<0 m>0 image upright

Page 16: Lecture 17 Ray Optics-3 Chapter 23 PHYSICS 270 Dennis Papadopoulos March 22, 2010.

EXAMPLE 23.10 Magnifying a flower

s<f

Page 17: Lecture 17 Ray Optics-3 Chapter 23 PHYSICS 270 Dennis Papadopoulos March 22, 2010.

Diverging Lenses

Thicker at the edges

Demagnification

Page 18: Lecture 17 Ray Optics-3 Chapter 23 PHYSICS 270 Dennis Papadopoulos March 22, 2010.

Diverging lenses Ray Tracing


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