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Chapter 34: Thin Lenses 1 Now consider refraction through this piece of glass: optic axis This is...

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Chapter 34: Thin Lenses 1 w consider refraction through this piece of gla optic axis This is called a “Double Convex Lens” converging light focal point refraction occurs here
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Page 1: Chapter 34: Thin Lenses 1 Now consider refraction through this piece of glass: optic axis This is called a “Double Convex Lens” converging light focal.

Chapter 34: Thin Lenses

1

Now consider refraction through this piece of glass:

opticaxis

This is called a “Double Convex Lens”

converging light

focal point

refraction occurs here

Page 2: Chapter 34: Thin Lenses 1 Now consider refraction through this piece of glass: optic axis This is called a “Double Convex Lens” converging light focal.

Chapter 34: Thin Lenses

2

Converging Lenses(convex)

Diverging Lenses(concave)

Page 3: Chapter 34: Thin Lenses 1 Now consider refraction through this piece of glass: optic axis This is called a “Double Convex Lens” converging light focal.

Chapter 34: Thin Lenses

3

Converging Lens

The focal point is visible because real rays go through it.

Diverging Lens

Where is the focal point for these 4 incoming rays?

Don’t confuse these reflections for something meaningful.

Page 4: Chapter 34: Thin Lenses 1 Now consider refraction through this piece of glass: optic axis This is called a “Double Convex Lens” converging light focal.

Chapter 34: Thin Lenses

4

Optical Ray Diagram: a line drawing depicting a small number of key light rays. For a lens, an optical ray diagram should include:

1. Parallel Ray. A ray parallel to the optic axis which passes through the object & the focal point.

2. Focal Ray. A ray that passes through both the focal point and the object.

3. Chief Ray. A ray that passes through both the center of the lens and the object.

These three rays intersect at the image.Note: we don’t use reflected rays in lens analysis.

Page 5: Chapter 34: Thin Lenses 1 Now consider refraction through this piece of glass: optic axis This is called a “Double Convex Lens” converging light focal.

Chapter 34: Thin Lenses

5

The Diverging Lens

parallel ray

virtual p

art

real p

art

Virtual part: where the refracted ray appears to come from.

f f

Page 6: Chapter 34: Thin Lenses 1 Now consider refraction through this piece of glass: optic axis This is called a “Double Convex Lens” converging light focal.

Chapter 34: Thin Lenses

6

The Diverging Lens

virtual part real part

focal ray

Virtual part: where the refracted ray appears to come from.

Page 7: Chapter 34: Thin Lenses 1 Now consider refraction through this piece of glass: optic axis This is called a “Double Convex Lens” converging light focal.

Chapter 34: Thin Lenses

7

The Diverging Lens

chief ray

The chief ray has no virtual part.

Page 8: Chapter 34: Thin Lenses 1 Now consider refraction through this piece of glass: optic axis This is called a “Double Convex Lens” converging light focal.

Chapter 34: Thin Lenses

8

Put all three rays together:

The three refracted rays have no intersection.

Page 9: Chapter 34: Thin Lenses 1 Now consider refraction through this piece of glass: optic axis This is called a “Double Convex Lens” converging light focal.

Chapter 34: Thin Lenses

9

Put all three rays together:

There is an intersection of the virtual parts.

Need virtual parts to find the image? Virtual image.

upright image

object

focalpoint

Page 10: Chapter 34: Thin Lenses 1 Now consider refraction through this piece of glass: optic axis This is called a “Double Convex Lens” converging light focal.

Chapter 34: Thin Lenses

10

Parallel ray

Chief rayFocal ray

so

f

si

a converging lens

The Thin Lens Equation

Page 11: Chapter 34: Thin Lenses 1 Now consider refraction through this piece of glass: optic axis This is called a “Double Convex Lens” converging light focal.

Chapter 34: Thin Lenses

11

Parallel ray

Chief rayFocal ray

a converging lens

Positive side forobject distance

Negative side forimage distancefocal length (e.g. diverging lens)

Positive side forimage distancefocal length

Opposite for mirrors

The Thin Lens Equation

Page 12: Chapter 34: Thin Lenses 1 Now consider refraction through this piece of glass: optic axis This is called a “Double Convex Lens” converging light focal.

Chapter 34: Thin Lenses

12

fss io

111

The Thin Lens Equation

“Strength” or “Power” of lens

fP

1

f, so and di all must have the same length units.

Units of P usually in [m-1] or rather [Diopters].

Pss io

11

Note: our book uses “P”. Other books use “S”.

Page 13: Chapter 34: Thin Lenses 1 Now consider refraction through this piece of glass: optic axis This is called a “Double Convex Lens” converging light focal.

Chapter 34: Thin Lenses

13

Why is 1/f called the “lens power”?

focal point at

light on the EFFECT NO has lens then the

0 f

1Prather or f if

(or sometimes “strength”)

“approaches”

Page 14: Chapter 34: Thin Lenses 1 Now consider refraction through this piece of glass: optic axis This is called a “Double Convex Lens” converging light focal.

Chapter 34: Thin Lenses

14

focal point very close to the lens

light on the EFFECT HUGE A has lens then the

f

1Prather or 0f if

Why is 1/f called the “lens power”?(or sometimes “strength”)

“approaches”

Page 15: Chapter 34: Thin Lenses 1 Now consider refraction through this piece of glass: optic axis This is called a “Double Convex Lens” converging light focal.

Chapter 34: Thin Lenses

15

Example 1: A lens focuses light from an object 2.75m away as an image 0.483m on the other side of the lens. What are the focal length, lens type and image type?

The lens is converging because: f>0

Converging lens: f>0Diverging lens: f<0

What is the image type?

meters 411.0

483.0

1

75.2

1111

f

mmssf io

Page 16: Chapter 34: Thin Lenses 1 Now consider refraction through this piece of glass: optic axis This is called a “Double Convex Lens” converging light focal.

Chapter 34: Thin Lenses

16

The image is real (si>0). Is it inverted or upright?

Ray diagram shows the image is: Real Inverted

True whenever the object is outside the focal point of a converging lens.

2.75 m

0.411m

0.483m

6 cm = 1m

Page 17: Chapter 34: Thin Lenses 1 Now consider refraction through this piece of glass: optic axis This is called a “Double Convex Lens” converging light focal.

Chapter 34: Thin Lenses

17

The ray diagram also shows the image is small.

hohi

Magnification:

o

i

o

i

d

d

h

hm

Minus sign indicates that real images are always inverted.

positive side for di and f

negative side for di and f

Page 18: Chapter 34: Thin Lenses 1 Now consider refraction through this piece of glass: optic axis This is called a “Double Convex Lens” converging light focal.

Chapter 34: Thin Lenses

18

How to do lens problems graphically

1. Use a full sheet – Landscape.2. Sketch the lens on the optic axis.3. Sketch the objects – correctly positioned.4. Show a scale. You might wish to show a

different scale for vertical and horizontal lengths

5. Sketch two principle rays per object and find the image.

6. Refraction occurs on the vertical center-line.

Page 19: Chapter 34: Thin Lenses 1 Now consider refraction through this piece of glass: optic axis This is called a “Double Convex Lens” converging light focal.

Chapter 34: Thin Lenses

19

Example 2: How far from a converging lens with a focal length of 25 cm should an object be placed to produce a real image which is the same size as the object?

cm 50s

s

2

s

1

s

1

cm 25

1

s

1

s

1

f

1

ooo

io

o

oss 1 s

s m want We i

o

i (Minus because all real images are inverted.)

si >0

Page 20: Chapter 34: Thin Lenses 1 Now consider refraction through this piece of glass: optic axis This is called a “Double Convex Lens” converging light focal.

Chapter 34: Thin Lenses

20

How to make a magnifying glass

What kind of lens has an upright image with m>1?

si <0

f

Place the object within the focal length of a converging lens.

1o

i

s

sm si negative

|si| > |so| image is farther from the

lens than the object


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