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Chapter 35
Chapter 35 -
- Refraction
Refraction
A PowerPoint Presentation by
Paul E. Tippens, Professor of Physics
Southern Polytechnic State University
A PowerPoint Presentation by
A PowerPoint Presentation by
Paul E. Tippens, Professor of Physics
Paul E. Tippens, Professor of Physics
Southern Polytechnic State University
Southern Polytechnic State University
© 2007
Objectives:
Objectives: After completing this
After completing this
module, you should be able to:
module, you should be able to:
•
• Define and apply the concept of the
Define and apply the concept of the index
index
of refraction
of refraction and discuss its effect on the
and discuss its effect on the
velocity and wavelength of light.
velocity and wavelength of light.
•
• Determine the changes in
Determine the changes in velocity
velocity and/or
and/or
wavelength
wavelength of light after refraction.
of light after refraction.
•
• Apply
Apply Snell
Snell’
’s law
s law to the solution of problems
to the solution of problems
involving the refraction of light.
involving the refraction of light.
•
• Define and apply the concepts of
Define and apply the concepts of total internal
total internal
reflection
reflection and the
and the critical angle
critical angle of incidence.
of incidence.
Refraction
Refraction
Water
Air
Refraction is the
bending of light as it
passes from one
medium into another.
Refraction is the
bending of light as it
passes from one
medium into another.
refraction
N
w
A
Note: the angle of
Note: the angle of
incidence
incidence 
A
A in air
in air
and the angle of
and the angle of
refraction
refraction 
A
A in water
in water
are each measured
are each measured
with the normal
with the normal N
N.
.
The incident and refracted
rays lie in the same plane
and are reversible.
The incident and refracted
The incident and refracted
rays lie in the same plane
rays lie in the same plane
and are reversible.
and are reversible.
Refraction Distorts Vision
Refraction Distorts Vision
Water
Air
Water
Air
The eye, believing that light travels in straight
lines, sees objects closer to the surface due to
refraction. Such distortions are common.
The eye, believing that light travels in straight
The eye, believing that light travels in straight
lines, sees objects closer to the surface due to
lines, sees objects closer to the surface due to
refraction. Such distortions are common.
refraction. Such distortions are common.
The Index of Refraction
The Index of Refraction
The index of refraction for a material is the ratio
of the velocity of light in a vacuum (3 x 108 m/s)
to the velocity through the material.
The
The index of refraction
index of refraction for a material is the ratio
for a material is the ratio
of the velocity of light in a vacuum (3 x 10
of the velocity of light in a vacuum (3 x 108
8 m/s)
m/s)
to the velocity through the material.
to the velocity through the material.
c
v
c
n
v

Index of refraction
c
n
v

Examples: Air n= 1; glass n = 1.5; Water n = 1.33
Examples: Air n= 1; glass n = 1.5; Water n = 1.33
Example 1.
Example 1. Light travels from air (
Light travels from air (n =
n = 1
1) into glass,
) into glass,
where its velocity reduces to only
where its velocity reduces to only 2 x 10
2 x 108
8 m/s
m/s.
.
What is the index of refraction for glass?
What is the index of refraction for glass?
8
8
3 x 10 m/s
2 x 10 m/s
c
n
v
 
vair = c
vG = 2 x 108 m/s
Glass
Air
For glass: n = 1.50
If the medium were
If the medium were water
water:
: n
nW
W =
= 1.33
1.33. Then
. Then
you should show that the velocity in water
you should show that the velocity in water
would be reduced from
would be reduced from c
c to
to 2.26 x 10
2.26 x 108
8 m/s
m/s.
.
Analogy for Refraction
Analogy for Refraction
Sand
Pavement
Air
Glass
Light bends into glass then returns along
original path much as a rolling axle would
when encountering a strip of mud.
Light bends into glass then returns along
Light bends into glass then returns along
original path much as a rolling axle would
original path much as a rolling axle would
when encountering a strip of mud.
when encountering a strip of mud.
3 x 108 m/s
3 x 108 m/s
2 x 108
m/s
vs < vp
Deriving Snell
Deriving Snell’
’s Law
s Law
Medium 1
Medium 2


 

Consider two light
Consider two light
rays. Velocities are
rays. Velocities are
v
v1
1 in medium 1
in medium 1
and
and v
v2
2 in med. 2.
in med. 2.
Segment
Segment R
R is common
is common
hypotenuse to two
hypotenuse to two rgt
rgt.
.
triangles. Verify shown
triangles. Verify shown
angles from geometry.
angles from geometry.
v1
v1t
v2
v2t 
1
1
R
R
1 2
1 2
sin ; sin
v t v t
R R
 
 
1
1 1
2
2 2
sin
sin
v t
v
R
v t v
R


 
Snell
Snell’
’s Law
s Law
1
2
Medium 1
Medium 2
The ratio of the sine of the
angle of incidence 1 to the
sine of the angle of refraction
2 is equal to the ratio of the
incident velocity v1 to the
refracted velocity v2 .
The ratio of the
The ratio of the sine
sine of the
of the
angle of incidence
angle of incidence 
1
1 to the
to the
sine
sine of the angle of refraction
of the angle of refraction

2
2 is equal to the ratio of the
is equal to the ratio of the
incident
incident velocity
velocity v
v1
1 to the
to the
refracted
refracted velocity
velocity v
v2
2 .
.
Snell’s
Law:
1 1
2 2
sin
sin
v
v



v1
v2
Example 2:
Example 2: A laser beam in a darkened room
A laser beam in a darkened room
strikes the surface of water at an angle of
strikes the surface of water at an angle of
30
300
0. The velocity in water is 2.26 x 10
. The velocity in water is 2.26 x 108
8 m/s.
m/s.
What is the angle of refraction?
What is the angle of refraction?
The incident angle is:
The incident angle is:

A
A = 90
= 900
0 –
– 30
300
0 = 60
= 600
0
sin
sin
A A
W W
v
v



8 0
8
sin (2 x 10 m/s)sin 60
sin
3 x 10 m/s
W A
W
A
v
v

   W = 35.30
W = 35.30
Air
Air
H2O
30
300
0
W

A
A
Snell
Snell’
’s Law and Refractive Index
s Law and Refractive Index
Another form of Snell
Another form of Snell’
’s law can be derived from
s law can be derived from
the definition of the index of refraction:
the definition of the index of refraction:
from which
c c
n v
v n
 
1 1 2
1
2 2 1
2
;
c
v v n
n
c
v v n
n
 
1 1 2
2 2 1
sin
sin
v n
v n


 
Snell
Snell’
’s law for
s law for
velocities and indices:
velocities and indices:
Medium 1
1
2
Medium 2
A Simplified Form of the Law
A Simplified Form of the Law
1 1 2
2 2 1
sin
sin
v n
v n


 
Since the indices of refraction for many common
Since the indices of refraction for many common
substances are usually available, Snell
substances are usually available, Snell’
’s law is
s law is
often written in the following manner:
often written in the following manner:
1 1 2 2
sin sin
n n
 

The product of the index of refraction and the
sine of the angle is the same in the refracted
medium as for the incident medium.
The product of the index of refraction and the
The product of the index of refraction and the
sine of the angle is the same in the refracted
sine of the angle is the same in the refracted
medium as for the incident medium.
medium as for the incident medium.
Example 3.
Example 3. Light travels through a block of glass,
Light travels through a block of glass,
then remerges into air. Find angle of emergence
then remerges into air. Find angle of emergence
for given information.
for given information.
Glass
Air
Air
Air
Air
n=1.5
First find
First find 
G
G inside glass:
inside glass:
sin sin
A A G G
n n
 

50
500
0
G

 0
sin (1.0)sin50
sin
1.50
A A
G
G
n
n

  
G = 30.70
G = 30.70
From geometry, note
From geometry, note
angle
angle 
G
G same for
same for
next interface.
next interface.
G
sin sin sin
A G G A
A A
n n n

 
 
Apply to each interface:
Apply to each interface:
e = 500
e = 500
Same as entrance angle!
Same as entrance angle!
Wavelength and Refraction
Wavelength and Refraction
The energy of light is determined by the frequency
The energy of light is determined by the frequency
of the EM waves, which remains constant as light
of the EM waves, which remains constant as light
passes into and out of a medium. (Recall
passes into and out of a medium. (Recall v = f
v = f
.
.)
)
Glass
Air n=1
n=1.5
A
G
fA= fG
G A
;
A A A G G G
v f v f
 
 
; ;
A A A A
G G G G
v f v
v f v
 
 
 
1 1 1
2 2 2
sin
sin
v
v
 
 
 
The Many Forms of Snell
The Many Forms of Snell’
’s Law:
s Law:
Refraction is affected by the index of refraction,
the velocity, and the wavelength. In general:
Refraction is affected by the index of refraction,
Refraction is affected by the index of refraction,
the velocity, and the wavelength. In general:
the velocity, and the wavelength. In general:
1 2 1 1
2 1 2 2
sin
sin
n v
n v
 
 
  
All the ratios are equal. It is helpful to recognize
that only the index n differs in the ratio order.
All the ratios are equal. It is helpful to recognize
that only the index n differs in the ratio order.
Snell’s
Law:
Example 4:
Example 4: A helium neon laser emits a beam of
A helium neon laser emits a beam of
wavelength
wavelength 632 nm
632 nm in air (
in air (n
nA
A = 1
= 1). What is the
). What is the
wavelength inside a slab of glass (
wavelength inside a slab of glass (n
nG
G = 1.5
= 1.5)?
)?
n
nG
G = 1.5;
= 1.5; 
A
A = 632 nm
= 632 nm
;
G
A A A
G
G A G
n n
n n
 


 
(1.0)(632 nm)
1.5
421 nm
G
  
Note that the light, if seen
Note that the light, if seen inside
inside the glass, would
the glass, would
be
be blue
blue. Of course it still appears red because it
. Of course it still appears red because it
returns to air before striking the eye.
returns to air before striking the eye.
Glass
Air
Air
Air
Air
n=1.5


G


G
Dispersion by a Prism
Dispersion by a Prism
Red
Orange
Yellow
Green
Blue
Indigo
Violet
Dispersion is the separation of white light into
its various spectral components. The colors
are refracted at different angles due to the
different indexes of refraction.
Dispersion
Dispersion is the separation of white light into
is the separation of white light into
its various spectral components. The colors
its various spectral components. The colors
are refracted at different angles due to the
are refracted at different angles due to the
different indexes of refraction.
different indexes of refraction.
Total Internal Reflection
Total Internal Reflection
Water
Air
light
The critical angle c is the
limiting angle of incidence
in a denser medium that
results in an angle of
refraction equal to 900.
The
The critical angle
critical angle 
c
c is the
is the
limiting angle of incidence
limiting angle of incidence
in a denser medium that
in a denser medium that
results in an angle of
results in an angle of
refraction equal to 90
refraction equal to 900
0.
.
When light passes at an angle from a medium of
When light passes at an angle from a medium of
higher index to one of lower index, the emerging
higher index to one of lower index, the emerging
ray bends away from the normal.
ray bends away from the normal.
When the angle reaches a
When the angle reaches a
certain maximum, it will be
certain maximum, it will be
reflected internally.
reflected internally.
i = r
Critical
angle

c
c
90
900
0
Example 5.
Example 5. Find the critical angle of incidence
Find the critical angle of incidence
from water to air.
from water to air.
For critical angle,
For critical angle, 
A
A = 90
= 900
0
n
nA
A = 1.0;
= 1.0; n
nW
W = 1.33
= 1.33
sin sin
W C A A
n n
 

0
sin90 (1)(1)
sin
1.33
A
C
w
n
n
  
Critical angle: c = 48.80 Water
Air

c
c
90
900
0
Critical angle
In general, for media where
In general, for media where
n
n1
1 >
> n
n2
2 we find that:
we find that:
1
2
sin C
n
n
 
Summary
Summary
1 2 1 1
2 1 2 2
sin
sin
n v
n v
 
 
  
Snell’s
Law:
Refraction is affected by the index of refraction,
the velocity, and the wavelength. In general:
Refraction is affected by the index of refraction,
Refraction is affected by the index of refraction,
the velocity, and the wavelength. In general:
the velocity, and the wavelength. In general:
c = 3 x 108 m/s
v
Index of refraction
c
n
v

Medium
n
Summary (Cont.)
Summary (Cont.)
The critical angle c is the
limiting angle of incidence
in a denser medium that
results in an angle of
refraction equal to 900.
The
The critical angle
critical angle 
c
c is the
is the
limiting angle of incidence
limiting angle of incidence
in a denser medium that
in a denser medium that
results in an angle of
results in an angle of
refraction equal to 90
refraction equal to 900
0.
.
In general, for media where
n1 > n2 we find that:
1
2
sin C
n
n
 
n1 > n2

c
c
90
900
0
Critical angle
n1
n2
CONCLUSION: Chapter 35
CONCLUSION: Chapter 35
Refraction
Refraction

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Refraction of Light-Notes.pdf

  • 1. Chapter 35 Chapter 35 - - Refraction Refraction A PowerPoint Presentation by Paul E. Tippens, Professor of Physics Southern Polytechnic State University A PowerPoint Presentation by A PowerPoint Presentation by Paul E. Tippens, Professor of Physics Paul E. Tippens, Professor of Physics Southern Polytechnic State University Southern Polytechnic State University © 2007
  • 2. Objectives: Objectives: After completing this After completing this module, you should be able to: module, you should be able to: • • Define and apply the concept of the Define and apply the concept of the index index of refraction of refraction and discuss its effect on the and discuss its effect on the velocity and wavelength of light. velocity and wavelength of light. • • Determine the changes in Determine the changes in velocity velocity and/or and/or wavelength wavelength of light after refraction. of light after refraction. • • Apply Apply Snell Snell’ ’s law s law to the solution of problems to the solution of problems involving the refraction of light. involving the refraction of light. • • Define and apply the concepts of Define and apply the concepts of total internal total internal reflection reflection and the and the critical angle critical angle of incidence. of incidence.
  • 3. Refraction Refraction Water Air Refraction is the bending of light as it passes from one medium into another. Refraction is the bending of light as it passes from one medium into another. refraction N w A Note: the angle of Note: the angle of incidence incidence  A A in air in air and the angle of and the angle of refraction refraction  A A in water in water are each measured are each measured with the normal with the normal N N. . The incident and refracted rays lie in the same plane and are reversible. The incident and refracted The incident and refracted rays lie in the same plane rays lie in the same plane and are reversible. and are reversible.
  • 4. Refraction Distorts Vision Refraction Distorts Vision Water Air Water Air The eye, believing that light travels in straight lines, sees objects closer to the surface due to refraction. Such distortions are common. The eye, believing that light travels in straight The eye, believing that light travels in straight lines, sees objects closer to the surface due to lines, sees objects closer to the surface due to refraction. Such distortions are common. refraction. Such distortions are common.
  • 5. The Index of Refraction The Index of Refraction The index of refraction for a material is the ratio of the velocity of light in a vacuum (3 x 108 m/s) to the velocity through the material. The The index of refraction index of refraction for a material is the ratio for a material is the ratio of the velocity of light in a vacuum (3 x 10 of the velocity of light in a vacuum (3 x 108 8 m/s) m/s) to the velocity through the material. to the velocity through the material. c v c n v  Index of refraction c n v  Examples: Air n= 1; glass n = 1.5; Water n = 1.33 Examples: Air n= 1; glass n = 1.5; Water n = 1.33
  • 6. Example 1. Example 1. Light travels from air ( Light travels from air (n = n = 1 1) into glass, ) into glass, where its velocity reduces to only where its velocity reduces to only 2 x 10 2 x 108 8 m/s m/s. . What is the index of refraction for glass? What is the index of refraction for glass? 8 8 3 x 10 m/s 2 x 10 m/s c n v   vair = c vG = 2 x 108 m/s Glass Air For glass: n = 1.50 If the medium were If the medium were water water: : n nW W = = 1.33 1.33. Then . Then you should show that the velocity in water you should show that the velocity in water would be reduced from would be reduced from c c to to 2.26 x 10 2.26 x 108 8 m/s m/s. .
  • 7. Analogy for Refraction Analogy for Refraction Sand Pavement Air Glass Light bends into glass then returns along original path much as a rolling axle would when encountering a strip of mud. Light bends into glass then returns along Light bends into glass then returns along original path much as a rolling axle would original path much as a rolling axle would when encountering a strip of mud. when encountering a strip of mud. 3 x 108 m/s 3 x 108 m/s 2 x 108 m/s vs < vp
  • 8. Deriving Snell Deriving Snell’ ’s Law s Law Medium 1 Medium 2      Consider two light Consider two light rays. Velocities are rays. Velocities are v v1 1 in medium 1 in medium 1 and and v v2 2 in med. 2. in med. 2. Segment Segment R R is common is common hypotenuse to two hypotenuse to two rgt rgt. . triangles. Verify shown triangles. Verify shown angles from geometry. angles from geometry. v1 v1t v2 v2t  1 1 R R 1 2 1 2 sin ; sin v t v t R R     1 1 1 2 2 2 sin sin v t v R v t v R    
  • 9. Snell Snell’ ’s Law s Law 1 2 Medium 1 Medium 2 The ratio of the sine of the angle of incidence 1 to the sine of the angle of refraction 2 is equal to the ratio of the incident velocity v1 to the refracted velocity v2 . The ratio of the The ratio of the sine sine of the of the angle of incidence angle of incidence  1 1 to the to the sine sine of the angle of refraction of the angle of refraction  2 2 is equal to the ratio of the is equal to the ratio of the incident incident velocity velocity v v1 1 to the to the refracted refracted velocity velocity v v2 2 . . Snell’s Law: 1 1 2 2 sin sin v v    v1 v2
  • 10. Example 2: Example 2: A laser beam in a darkened room A laser beam in a darkened room strikes the surface of water at an angle of strikes the surface of water at an angle of 30 300 0. The velocity in water is 2.26 x 10 . The velocity in water is 2.26 x 108 8 m/s. m/s. What is the angle of refraction? What is the angle of refraction? The incident angle is: The incident angle is:  A A = 90 = 900 0 – – 30 300 0 = 60 = 600 0 sin sin A A W W v v    8 0 8 sin (2 x 10 m/s)sin 60 sin 3 x 10 m/s W A W A v v     W = 35.30 W = 35.30 Air Air H2O 30 300 0 W  A A
  • 11. Snell Snell’ ’s Law and Refractive Index s Law and Refractive Index Another form of Snell Another form of Snell’ ’s law can be derived from s law can be derived from the definition of the index of refraction: the definition of the index of refraction: from which c c n v v n   1 1 2 1 2 2 1 2 ; c v v n n c v v n n   1 1 2 2 2 1 sin sin v n v n     Snell Snell’ ’s law for s law for velocities and indices: velocities and indices: Medium 1 1 2 Medium 2
  • 12. A Simplified Form of the Law A Simplified Form of the Law 1 1 2 2 2 1 sin sin v n v n     Since the indices of refraction for many common Since the indices of refraction for many common substances are usually available, Snell substances are usually available, Snell’ ’s law is s law is often written in the following manner: often written in the following manner: 1 1 2 2 sin sin n n    The product of the index of refraction and the sine of the angle is the same in the refracted medium as for the incident medium. The product of the index of refraction and the The product of the index of refraction and the sine of the angle is the same in the refracted sine of the angle is the same in the refracted medium as for the incident medium. medium as for the incident medium.
  • 13. Example 3. Example 3. Light travels through a block of glass, Light travels through a block of glass, then remerges into air. Find angle of emergence then remerges into air. Find angle of emergence for given information. for given information. Glass Air Air Air Air n=1.5 First find First find  G G inside glass: inside glass: sin sin A A G G n n    50 500 0 G   0 sin (1.0)sin50 sin 1.50 A A G G n n     G = 30.70 G = 30.70 From geometry, note From geometry, note angle angle  G G same for same for next interface. next interface. G sin sin sin A G G A A A n n n      Apply to each interface: Apply to each interface: e = 500 e = 500 Same as entrance angle! Same as entrance angle!
  • 14. Wavelength and Refraction Wavelength and Refraction The energy of light is determined by the frequency The energy of light is determined by the frequency of the EM waves, which remains constant as light of the EM waves, which remains constant as light passes into and out of a medium. (Recall passes into and out of a medium. (Recall v = f v = f . .) ) Glass Air n=1 n=1.5 A G fA= fG G A ; A A A G G G v f v f     ; ; A A A A G G G G v f v v f v       1 1 1 2 2 2 sin sin v v      
  • 15. The Many Forms of Snell The Many Forms of Snell’ ’s Law: s Law: Refraction is affected by the index of refraction, the velocity, and the wavelength. In general: Refraction is affected by the index of refraction, Refraction is affected by the index of refraction, the velocity, and the wavelength. In general: the velocity, and the wavelength. In general: 1 2 1 1 2 1 2 2 sin sin n v n v        All the ratios are equal. It is helpful to recognize that only the index n differs in the ratio order. All the ratios are equal. It is helpful to recognize that only the index n differs in the ratio order. Snell’s Law:
  • 16. Example 4: Example 4: A helium neon laser emits a beam of A helium neon laser emits a beam of wavelength wavelength 632 nm 632 nm in air ( in air (n nA A = 1 = 1). What is the ). What is the wavelength inside a slab of glass ( wavelength inside a slab of glass (n nG G = 1.5 = 1.5)? )? n nG G = 1.5; = 1.5;  A A = 632 nm = 632 nm ; G A A A G G A G n n n n       (1.0)(632 nm) 1.5 421 nm G    Note that the light, if seen Note that the light, if seen inside inside the glass, would the glass, would be be blue blue. Of course it still appears red because it . Of course it still appears red because it returns to air before striking the eye. returns to air before striking the eye. Glass Air Air Air Air n=1.5   G   G
  • 17. Dispersion by a Prism Dispersion by a Prism Red Orange Yellow Green Blue Indigo Violet Dispersion is the separation of white light into its various spectral components. The colors are refracted at different angles due to the different indexes of refraction. Dispersion Dispersion is the separation of white light into is the separation of white light into its various spectral components. The colors its various spectral components. The colors are refracted at different angles due to the are refracted at different angles due to the different indexes of refraction. different indexes of refraction.
  • 18. Total Internal Reflection Total Internal Reflection Water Air light The critical angle c is the limiting angle of incidence in a denser medium that results in an angle of refraction equal to 900. The The critical angle critical angle  c c is the is the limiting angle of incidence limiting angle of incidence in a denser medium that in a denser medium that results in an angle of results in an angle of refraction equal to 90 refraction equal to 900 0. . When light passes at an angle from a medium of When light passes at an angle from a medium of higher index to one of lower index, the emerging higher index to one of lower index, the emerging ray bends away from the normal. ray bends away from the normal. When the angle reaches a When the angle reaches a certain maximum, it will be certain maximum, it will be reflected internally. reflected internally. i = r Critical angle  c c 90 900 0
  • 19. Example 5. Example 5. Find the critical angle of incidence Find the critical angle of incidence from water to air. from water to air. For critical angle, For critical angle,  A A = 90 = 900 0 n nA A = 1.0; = 1.0; n nW W = 1.33 = 1.33 sin sin W C A A n n    0 sin90 (1)(1) sin 1.33 A C w n n    Critical angle: c = 48.80 Water Air  c c 90 900 0 Critical angle In general, for media where In general, for media where n n1 1 > > n n2 2 we find that: we find that: 1 2 sin C n n  
  • 20. Summary Summary 1 2 1 1 2 1 2 2 sin sin n v n v        Snell’s Law: Refraction is affected by the index of refraction, the velocity, and the wavelength. In general: Refraction is affected by the index of refraction, Refraction is affected by the index of refraction, the velocity, and the wavelength. In general: the velocity, and the wavelength. In general: c = 3 x 108 m/s v Index of refraction c n v  Medium n
  • 21. Summary (Cont.) Summary (Cont.) The critical angle c is the limiting angle of incidence in a denser medium that results in an angle of refraction equal to 900. The The critical angle critical angle  c c is the is the limiting angle of incidence limiting angle of incidence in a denser medium that in a denser medium that results in an angle of results in an angle of refraction equal to 90 refraction equal to 900 0. . In general, for media where n1 > n2 we find that: 1 2 sin C n n   n1 > n2  c c 90 900 0 Critical angle n1 n2
  • 22. CONCLUSION: Chapter 35 CONCLUSION: Chapter 35 Refraction Refraction