10. Refraction
• Light also goes through some things
• The presence of material slows light’s progress
– interactions with electrical properties of atoms
• The “light slowing factor” is called the index of
refraction
– glass has n = 1.52 (meaning that light travels about 1.5
times slower in glass than in vacuum)
– water has n = 1.33
– air has n = 1.00028
11. glass; n2 = 1.5
air; n1 = 1.0
A
B
Refraction at a plane surface
Light bends at interface
between refractive
indices
Bends more the larger the
difference in refractive index
normal line
12. Convex Glass Surface
C
axis
A convex surface is called “converging” because parallel rays converge
towards one another
AIR (fast) GLASS (slow)
normal line
fast to slow bends
towards the normal
13. Convex Glass Surface
Caxis
The surface is converging for both air to glass rays and glass to air rays
AIRGLASS
normal line
slow to fast bends
away from the normal
14. Caxis
A concave surface is called “diverging” because parallel rays diverge
away from one another
Concave Glass Surface
AIR GLASS
15. C axis
Again, the surface is diverging for both air to glass rays and glass to
air rays
Concave Glass Surface
AIRGLASS
18. Converging Lens
• The focal point of a curved
mirror was the image point
of a distant star
– It is the same for a lens.
– The focal point of a converging
lens is where the incoming
rays from a distant star all
intersect.
• A distant star is used to
guarantee that the incoming
rays are parallel
Focal point
Focal distance
20. F
Similarly to a spherical mirror, incoming parallel rays
are deflected through the focal point
21. Thin Lenses
• Just as the ray tracing for mirrors is approximate and only
accurate for certain situations, the ray tracing for lenses is
accurate only for what are called “thin lenses”
F’F
thickness of lens
distance to focal point
23. Converging Lens: Ray Tracing Rules
Rule 1:
Similarly to a spherical mirror, incoming parallel rays are deflected
through the focal point.
FF
24. Converging Lens: Ray Tracing Rules
Rule 2:
Rays passing through the center of the lens are undeflected, they
continue straight through without being bent. Several rays are
shown here as examples.
FF
25. Converging Lens: Ray Tracing Rules
Rule 3:
The reverse of Rule 1, rays passing through the focal point are
deflected to exit parallel to the axis
FF
27. The incident light ray from the object
that is parallel to the principal axis will
be refracted passing through the
principal focal point after passing
through the optic axis.
Parallel Ray
35. F F’2F 2F’
(1) Locate the image and
(2) Describe its characteristics
Focal length = 5 cm
Object’s location = 10 cm
Object’s height = 3 cm
Lens’ height = 8 cm
36. F F’2F 2F’
(1) Locate the image and
(2) Describe its characteristics
Focal length = 5 cm
Object’s location = 5 cm
Object’s height = 1 cm
Lens’ height = 8 cm
38. F’F
In diverging lens, parallel rays are deflected such that when extended
backwards, they appear to be coming from the focal point on the other side.
DIVERGING LENS
40. Diverging Lens: Ray Tracing
F’F
Parallel rays are deflected so they appear to be coming from the focal
point in front of the lens.
41. Diverging Lens: Ray Tracing
F’F
Just like for converging lenses, rays that pass through the center of
the lens continue undeflected (straight) through the lens.
42. Diverging Lens: Ray Tracing
F’F
Rays that, if extended, would pass through the focal point on the
other side of the lens, are deflected to be parallel to the axis.
44. The incident light ray from the object
that is parallel to the principal axis will
be refracted as if it came from the
secondary focal point.
Parallel Ray
51. Diverging Lens: Image Formation
F’F
The image is virtual*, reduced, and right side up.
52. F F’2F 2F’
(1) Locate the image and
(2) Describe its characteristics
Focal length = 5 cm
Object’s location = 10 cm
Object’s height = 3 cm
Lens’ height = 8 cm
53. F F’2F 2F’
(1) Locate the image and
(2) Describe its characteristics
Focal length = 5 cm
Object’s location = 5 cm
Object’s height = 1 cm
Lens’ height = 8 cm
55. Corrective Lenses: Myopia
To correct myopia (nearsightedness), a diverging lens creates an
intermediate image of a distant star at your far point so that your eye
can see it even though the star is beyond your far point.
56. Corrective Lenses: Myopia
To correct myopia (nearsightedness), a diverging lens creates an
intermediate image of a distant star at your far point so that your eye
can see it even though the star is beyond your far point.
far point
image of distant object
57. Corrective Lenses: Hyperopia
To correct farsightedness your contact lens creates an (intermediate)
image of a book 25 cm away at your near point so that your
farsighted eye can see it even though the book is closer than your
near point
25 cmnear point
58. Corrective Lenses: Hyperopia
To correct farsightedness your contact lens creates an (intermediate)
image of a book 25 cm away at your near point so that your
farsighted eye can see it even though the book is closer than your
near point
near point 25 cm
focal point of corrective lens
Editor's Notes
Note that a lens has a focal point on both sides of the lens, as compared to a mirror that only has one focal point
A lens is considered “thin” if the thickness of the lens is much less than the distance from the lens to the focal point.