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Chapter 33
Chapter 33 -
- Light and
Light and
Illumination
Illumination
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
Define light
light, discuss its properties, and give
, discuss its properties, and give
the range of wavelengths for visible spectrum.
the range of wavelengths for visible spectrum.
•
• Apply the relationship between
Apply the relationship between frequencies
frequencies
and
and wavelengths
wavelengths for optical waves.
for optical waves.
•
• Define and apply the concepts of
Define and apply the concepts of luminous
luminous
flux
flux,
, luminous intensity
luminous intensity, and
, and illumination
illumination.
.
•
• Solve problems similar to those presented in
Solve problems similar to those presented in
this module.
this module.
A Beginning Definition
A Beginning Definition
All objects are emitting
All objects are emitting
and absorbing EM
and absorbing EM radia
radia-
-
tion
tion. Consider a poker
. Consider a poker
placed in a fire.
placed in a fire.
As heating occurs, the
As heating occurs, the
emitted EM waves have
emitted EM waves have
higher energy and
higher energy and
eventually become visible.
eventually become visible.
First red . . . then white.
First red . . . then white.
3
4
2
1
Light may be defined as electromagnetic radiation
that is capable of affecting the sense of sight.
Light
Light may be defined as electromagnetic radiation
may be defined as electromagnetic radiation
that is capable of affecting the sense of sight.
that is capable of affecting the sense of sight.
Electromagnetic Waves
Electromagnetic Waves
c
c
E
E
B
B
Electric
Electric E
E
Magnetic
Magnetic B
B
Wave Properties:
Wave Properties:
1.
1. Waves travel at the
Waves travel at the
speed of light
speed of light c
c.
.
2.
2. Perpendicular electric
Perpendicular electric
and magnetic fields.
and magnetic fields.
3.
3. Require no medium
Require no medium
for propagation.
for propagation.
For a complete review of the electromagnetic
properties, you should study module 32C.
For a complete review of the electromagnetic
properties, you should study module 32C.
3 x 10
3 x 108
8 m/s
m/s
The Wavelengths of Light
The Wavelengths of Light
The electromagnetic spectrum spreads over a
tremendous range of frequencies or wavelengths.
The wavelength  is related to the frequency f:
The electromagnetic spectrum spreads over a
The electromagnetic spectrum spreads over a
tremendous range of frequencies or wavelengths.
tremendous range of frequencies or wavelengths.
The
The wavelength
wavelength 
 is related to the
is related to the frequency
frequency f
f:
:
c = fc = 3 x 108 m/s
c = fc = 3 x 108 m/s
Those EM waves that are visible (light) have wave
Those EM waves that are visible (light) have wave-
-
lengths that range from 0.00004 to 0.00007 cm.
lengths that range from 0.00004 to 0.00007 cm.
Red,
Red, 

0.00007 cm
0.00007 cm
Violet,
Violet, 

0.00004 cm
0.00004 cm
The EM Spectrum
The EM Spectrum
A wavelength of one
A wavelength of one
nanometer 1 nm is:
nanometer 1 nm is:
1 nm = 1 x 10-9 m
1 nm = 1 x 10-9 m
Red 700 nm
Red 700 nm 
 Violet 400 nm
Violet 400 nm
c = fc = 3 x 108 m/s
c = fc = 3 x 108 m/s
1024
1023
1022
1021
1020
1019
1018
1017
1016
1015
1014
1013
1012
1011
1010
109
108
107
106
105
104
Frequency wavelength
f (Hz) nm)
10-7
10-6
10-4
10-3
10-1
1
10
102
103
104
105
106
107
108
109
1010
1011
1012
1013
Gamma rays
X-rays
Infrared rays
Short Radio
waves
Broadcast Radio
Long Radio
waves
Ultraviolet
400 nm
400 nm 
 700 nm
700 nm
Visible Spectrum
Visible Spectrum
Example 1.
Example 1. Light from a Helium
Light from a Helium-
-Neon laser
Neon laser
has a wavelength of
has a wavelength of 632 nm
632 nm. What is the
. What is the
frequency of this wave?
frequency of this wave?
8
-9
3 x 10 m/s
632 x 10 m
c
c f f


  
f = 4.75 x 1014 Hz
f = 4.75 x 1014 Hz Red light
Red light
The Helium Neon Laser
The Helium Neon Laser Wavelength
Wavelength

 = 632 nm
= 632 nm
Laser
Properties of Light
Properties of Light
• Rectilinear propagation: Light travels in
straight lines.
• Reflection: Light striking a smooth surface
turns back into the original medium.
• Refraction: Light bends when entering a
transparent medium.
Any study of the nature of light must
explain the following observed properties:
Any study of the nature of light must
Any study of the nature of light must
explain the following observed properties:
explain the following observed properties:
The Nature of Light
The Nature of Light
Physicists have studied light for centuries, finding
that it sometimes behaves as a particle and
sometimes as a wave. Actually, both are correct!
Physicists have studied light for centuries, finding
Physicists have studied light for centuries, finding
that it sometimes behaves as a particle and
that it sometimes behaves as a particle and
sometimes as a wave. Actually, both are correct!
sometimes as a wave. Actually, both are correct!
Reflection and
Reflection and
rectilinear propagation
rectilinear propagation
(straight line path)
(straight line path)
Dispersion of white
Dispersion of white
light into colors.
light into colors.
Photons and Light Rays
Photons and Light Rays
Light may be thought of as little bundles of waves
Light may be thought of as little bundles of waves
emitted in discrete packets called
emitted in discrete packets called photons
photons.
.
photons
photons
The wave treatment uses
The wave treatment uses rays
rays to show
to show
the direction of advancing wave fronts.
the direction of advancing wave fronts.
Light
Light
ray
ray
Light rays are
convenient for
describing how
light behaves.
Light rays are
Light rays are
convenient for
convenient for
describing how
describing how
light behaves.
light behaves.
Light Rays and Shadows
Light Rays and Shadows
A geometric analysis may be made of shadows
A geometric analysis may be made of shadows
by tracing light rays from a point light source:
by tracing light rays from a point light source:
shadow
shadow
screen
screen
Point
Point
source
source
The dimensions of the shadow can be found
by using geometry and known distances.
The dimensions of the shadow can be found
by using geometry and known distances.
Example 2:
Example 2: The diameter of the ball is
The diameter of the ball is 4 cm
4 cm
and it is located
and it is located 20 cm
20 cm from the point light
from the point light
source. If the screen is
source. If the screen is 80 cm
80 cm from the
from the
source, what is the diameter of the shadow?
source, what is the diameter of the shadow?
4 cm
20 cm
80 cm
h
The ratio of
shadow to
the source
is same as
that of ball
to source.
Therefore:
The ratio of
The ratio of
shadow to
shadow to
the source
the source
is same as
is same as
that of ball
that of ball
to source.
to source.
Therefore:
Therefore:
(4 cm)(80 cm)
20 cm
h  h = 16 cm
4 cm
80 cm 20 cm
h

Shadows of Extended Objects
Shadows of Extended Objects
Extended
Extended
source
source
penumbra
penumbra
umbra
umbra
The
The umbra
umbra is the region where no light reaches
is the region where no light reaches
the screen.
the screen.
•
• The
The penumbra
penumbra is the outer area where
is the outer area where
only part of the light reaches the screen.
only part of the light reaches the screen.
•
• The
The umbra
umbra is the region where no light
is the region where no light
reaches the screen.
reaches the screen.
The Sensitivity Curve
The Sensitivity Curve
Sensitivity curve
Sensitivity curve
Wavelength
Wavelength 

Sensitivity
Sensitivity
Human eyes are not
Human eyes are not
equally sensitive to
equally sensitive to
all colors.
all colors.
Eyes are most
Eyes are most sensi
sensi-
-
tive
tive in the mid
in the mid-
-range
range
near
near 
= 555 nm
= 555 nm.
.
555 nm
555 nm
400 nm
400 nm 700 nm
700 nm
40 W
40 W 40 W
40 W
Yellow light appears brighter
to the eye than does red light.
Yellow
Yellow light appears brighter
light appears brighter
to the eye than does
to the eye than does red
red light.
light.
Luminous Flux
Luminous Flux
Luminous flux
Luminous flux is the portion of total radiant power
is the portion of total radiant power
that is capable of affecting the sense of sight.
that is capable of affecting the sense of sight.
Typically only about 10%
Typically only about 10%
of the power (flux) emitted
of the power (flux) emitted
from a light bulb falls in
from a light bulb falls in
the visible region.
the visible region.
The unit for luminous flux is the
The unit for luminous flux is the lumen
lumen which
which
will be given a quantitative definition later.
will be given a quantitative definition later.
A Solid Angle: Steradians
A Solid Angle: Steradians
Working with luminous flux requires the use of a
solid angle measure called the steradian (sr).
Working with luminous flux requires the use of a
solid angle measure called the steradian (sr).

A
R
The
Steradian 2
A
R
 
A solid angle of one
steradian (1 sr) is
subtended at the
center of a sphere
by an area A equal
to the square of its
radius ( R2 ).
A solid angle of one
A solid angle of one
steradian
steradian (
(1
1 sr
sr) is
) is
subtended at the
subtended at the
center of a sphere
center of a sphere
by an area
by an area A
A equal
equal
to the square of its
to the square of its
radius (
radius ( R
R2
2 ).
).
Example 3.
Example 3. What solid angle is subtended at
What solid angle is subtended at
the center of a sphere by an area of
the center of a sphere by an area of 1.6 m
1.6 m2
2?
?
The radius of the sphere is
The radius of the sphere is 5 m
5 m.
.

A
1.6 m2
R
5 m
The
Steradian 2
A
R
 
2
2
1.60 m
(5.00 m)
 
2
A
R
 
 = 0.00640 sr
 = 0.00640 sr
The Lumen as a Unit of Flux
The Lumen as a Unit of Flux
One
One lumen
lumen (lm)
(lm) is the
is the luminous flux
luminous flux emitted from
emitted from
a
a 1/60 cm
1/60 cm2
2 opening in a standard source and
opening in a standard source and
included in a solid angle of
included in a solid angle of one steradian
one steradian (1
(1 sr
sr).
).
In practice, sources of light are usually rated
In practice, sources of light are usually rated
by comparison to a commercially prepared
by comparison to a commercially prepared
standard light source.
standard light source.
A typical
A typical 100
100-
-W
W incandescent
incandescent
light bulb emits a total radiant
light bulb emits a total radiant
power of about
power of about 1750 lm
1750 lm. This is
. This is
for light emitted in all directions.
for light emitted in all directions.
The Lumen in Power Units
The Lumen in Power Units
Recalling that luminous flux is really radiant
Recalling that luminous flux is really radiant
power allows us to define the lumen as follows:
power allows us to define the lumen as follows:
One lumen is equal to 1/680 W of yellow-
green light of wavelength 555 nm.
One lumen is equal to 1/680 W of yellow
One lumen is equal to 1/680 W of yellow-
-
green light of wavelength 555 nm.
green light of wavelength 555 nm.
Wavelength
Wavelength 

Sensitivity curve
Sensitivity curve
A disadvantage of this
A disadvantage of this
approach is the need to
approach is the need to
refer to sensitivity curves
refer to sensitivity curves
to determine the flux for
to determine the flux for
different colors of light.
different colors of light.
Luminous Intensity
Luminous Intensity
The
The luminous intensity
luminous intensity I
I for a light source
for a light source
is the luminous flux per unit solid angle.
is the luminous flux per unit solid angle.

 F
I 

Luminous intensity:
F
I 

Unit is the candela (cd)
A source having an intensity of one candela
emits a flux of one lumen per steradian.
A source having an intensity of one candela
emits a flux of one lumen per steradian.
Total flux for Isotropic Source
Total flux for Isotropic Source

 R
R
3 m
3 m
An isotropic source emits in
An isotropic source emits in
all
all directions; i.e., over a
directions; i.e., over a
solid angle of
solid angle of 4
4
 steradians
steradians.
.
Total flux: F = 4I
Total flux: F = 4I
The flux confined to area A is:
The flux confined to area A is:
F = I A
F = I A

= 4
= 4
 sr
sr
Thus, for such
Thus, for such
a source, the
a source, the
intensity is:
intensity is: 4
F F
I

 

Example 4.
Example 4. A
A 30
30 cd
cd spotlight is located
spotlight is located 3 m
3 m
above a table. The beam is focused on a surface
above a table. The beam is focused on a surface
area of
area of 0.4 m
0.4 m2
2. Find the intensity of the beam.
. Find the intensity of the beam.
Total flux: F = 4I
Total flux: F = 4I
F
FT
T = 4
= 4
(30
(30 cd
cd) = 377 lm
) = 377 lm 
 R
R
3 m
3 m
The luminous intensity of
The luminous intensity of
the beam depends on
the beam depends on 

2
2 2
0.4 m
; 0.0444 sr
(3 m)
A
R
    
754 lm
0.0444 sr
F
I  

Beam Intensity:
Beam Intensity:
I = 8490 cd
I = 8490 cd
Illumination of a Surface
Illumination of a Surface
The illumination E of a surface A is defined as
the luminous flux per unit area (F/A) in lumens
per square meter which is renamed a lux (lx).
The
The illumination
illumination E
E of a surface
of a surface A
A is defined as
is defined as
the luminous flux per unit area (
the luminous flux per unit area (F/A
F/A) in
) in lumens
lumens
per square meter
per square meter which is renamed a
which is renamed a lux
lux (lx)
(lx).
.
Unit: lux (lx)
F
E
A

An illumination of one lux
occurs when a flux of
one lumen falls on an
area of one square
meter.
An illumination of one lux
occurs when a flux of
one lumen falls on an
area of one square
meter.


R
R
Area
Area A
A
Illumination,
Illumination, E
E
Illumination Based on Intensity
Illumination Based on Intensity
 R
Area A
; ;
F F
E I F I
A
   

2
but so that
I A
E
A R

  
2
Illumination,
I
E
R
 This equation applies for
perpendicular surfaces.
The illumination E of a surface is directly
proportional to the intensity I and inversely
proportional to the square of the distance R.
The
The illumination
illumination E
E of a surface is directly
of a surface is directly
proportional to the
proportional to the intensity
intensity I
I and inversely
and inversely
proportional to the
proportional to the square
square of the
of the distance R
distance R.
.
Example 5.
Example 5. A
A 400
400-
-cd
cd light is located
light is located 2.4 m
2.4 m
from a tabletop of area
from a tabletop of area 1.2 m
1.2 m2
2. What is the
. What is the
illumination and what flux
illumination and what flux F
F falls on the table?
falls on the table?
 R
2 2
400 cd
(2.40 m)
I
E
R
 
E = 69.4 lx
Illumination:
Illumination:
Now, recalling that
Now, recalling that E = F/A
E = F/A, we find
, we find F
F from:
from:
F = EA =
F = EA = (69.4 lx)(1.20 m
(69.4 lx)(1.20 m2
2)
) F = 93.3 lm
The Inverse Square Relationship
The Inverse Square Relationship
2
I
E
R

E/9
E/4
E
3 m
2 m
1 m
1 m2
4 m2
9 m2
If the intensity is 36 lx at 1 m, it will
be 9 lx at 2 m and only 4 lx at 3 m.
Summary
Summary
Light may be defined as electromagnetic radiation
that is capable of affecting the sense of sight.
Light
Light may be defined as electromagnetic radiation
may be defined as electromagnetic radiation
that is capable of affecting the sense of sight.
that is capable of affecting the sense of sight.
• Rectilinear propagation
• Reflection
• Refraction c = fc = 3 x 108 m/s
c = fc = 3 x 108 m/s
General Properties of Light:
Red,
Red, 

700 nm
700 nm
Violet,
Violet, 

400 nm
400 nm
Summary (Continued)
Summary (Continued)
Luminous flux
Luminous flux is the portion of total radiant power
is the portion of total radiant power
that is capable of affecting the sense of sight.
that is capable of affecting the sense of sight.
Extended
Extended
source
source
penumbra
penumbra
umbra
umbra
The formation of shadows:
The formation of shadows:
Summary (Continued)
Summary (Continued)
Unit: lux (lx)
F
E
A

Total flux: F = 4I
Total flux: F = 4I
Luminous intensity:
F
I 

Unit is the candela (cd)

A
R
The
Steradian 2
A
R
 
Summary (Cont.)
Summary (Cont.)


R
R
Area
Area A
A
Illumination,
Illumination, E
E
2
Illumination,
I
E
R

E/9
E/4
E
3 m
2 m
1 m
1 m2
4 m2
9 m2
CONCLUSION: Chapter 33
CONCLUSION: Chapter 33
Light and Illumination
Light and Illumination

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Light.pdf

  • 1. Chapter 33 Chapter 33 - - Light and Light and Illumination Illumination 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 Define light light, discuss its properties, and give , discuss its properties, and give the range of wavelengths for visible spectrum. the range of wavelengths for visible spectrum. • • Apply the relationship between Apply the relationship between frequencies frequencies and and wavelengths wavelengths for optical waves. for optical waves. • • Define and apply the concepts of Define and apply the concepts of luminous luminous flux flux, , luminous intensity luminous intensity, and , and illumination illumination. . • • Solve problems similar to those presented in Solve problems similar to those presented in this module. this module.
  • 3. A Beginning Definition A Beginning Definition All objects are emitting All objects are emitting and absorbing EM and absorbing EM radia radia- - tion tion. Consider a poker . Consider a poker placed in a fire. placed in a fire. As heating occurs, the As heating occurs, the emitted EM waves have emitted EM waves have higher energy and higher energy and eventually become visible. eventually become visible. First red . . . then white. First red . . . then white. 3 4 2 1 Light may be defined as electromagnetic radiation that is capable of affecting the sense of sight. Light Light may be defined as electromagnetic radiation may be defined as electromagnetic radiation that is capable of affecting the sense of sight. that is capable of affecting the sense of sight.
  • 4. Electromagnetic Waves Electromagnetic Waves c c E E B B Electric Electric E E Magnetic Magnetic B B Wave Properties: Wave Properties: 1. 1. Waves travel at the Waves travel at the speed of light speed of light c c. . 2. 2. Perpendicular electric Perpendicular electric and magnetic fields. and magnetic fields. 3. 3. Require no medium Require no medium for propagation. for propagation. For a complete review of the electromagnetic properties, you should study module 32C. For a complete review of the electromagnetic properties, you should study module 32C. 3 x 10 3 x 108 8 m/s m/s
  • 5. The Wavelengths of Light The Wavelengths of Light The electromagnetic spectrum spreads over a tremendous range of frequencies or wavelengths. The wavelength  is related to the frequency f: The electromagnetic spectrum spreads over a The electromagnetic spectrum spreads over a tremendous range of frequencies or wavelengths. tremendous range of frequencies or wavelengths. The The wavelength wavelength   is related to the is related to the frequency frequency f f: : c = fc = 3 x 108 m/s c = fc = 3 x 108 m/s Those EM waves that are visible (light) have wave Those EM waves that are visible (light) have wave- - lengths that range from 0.00004 to 0.00007 cm. lengths that range from 0.00004 to 0.00007 cm. Red, Red,   0.00007 cm 0.00007 cm Violet, Violet,   0.00004 cm 0.00004 cm
  • 6. The EM Spectrum The EM Spectrum A wavelength of one A wavelength of one nanometer 1 nm is: nanometer 1 nm is: 1 nm = 1 x 10-9 m 1 nm = 1 x 10-9 m Red 700 nm Red 700 nm   Violet 400 nm Violet 400 nm c = fc = 3 x 108 m/s c = fc = 3 x 108 m/s 1024 1023 1022 1021 1020 1019 1018 1017 1016 1015 1014 1013 1012 1011 1010 109 108 107 106 105 104 Frequency wavelength f (Hz) nm) 10-7 10-6 10-4 10-3 10-1 1 10 102 103 104 105 106 107 108 109 1010 1011 1012 1013 Gamma rays X-rays Infrared rays Short Radio waves Broadcast Radio Long Radio waves Ultraviolet 400 nm 400 nm   700 nm 700 nm Visible Spectrum Visible Spectrum
  • 7. Example 1. Example 1. Light from a Helium Light from a Helium- -Neon laser Neon laser has a wavelength of has a wavelength of 632 nm 632 nm. What is the . What is the frequency of this wave? frequency of this wave? 8 -9 3 x 10 m/s 632 x 10 m c c f f      f = 4.75 x 1014 Hz f = 4.75 x 1014 Hz Red light Red light The Helium Neon Laser The Helium Neon Laser Wavelength Wavelength   = 632 nm = 632 nm Laser
  • 8. Properties of Light Properties of Light • Rectilinear propagation: Light travels in straight lines. • Reflection: Light striking a smooth surface turns back into the original medium. • Refraction: Light bends when entering a transparent medium. Any study of the nature of light must explain the following observed properties: Any study of the nature of light must Any study of the nature of light must explain the following observed properties: explain the following observed properties:
  • 9. The Nature of Light The Nature of Light Physicists have studied light for centuries, finding that it sometimes behaves as a particle and sometimes as a wave. Actually, both are correct! Physicists have studied light for centuries, finding Physicists have studied light for centuries, finding that it sometimes behaves as a particle and that it sometimes behaves as a particle and sometimes as a wave. Actually, both are correct! sometimes as a wave. Actually, both are correct! Reflection and Reflection and rectilinear propagation rectilinear propagation (straight line path) (straight line path) Dispersion of white Dispersion of white light into colors. light into colors.
  • 10. Photons and Light Rays Photons and Light Rays Light may be thought of as little bundles of waves Light may be thought of as little bundles of waves emitted in discrete packets called emitted in discrete packets called photons photons. . photons photons The wave treatment uses The wave treatment uses rays rays to show to show the direction of advancing wave fronts. the direction of advancing wave fronts. Light Light ray ray Light rays are convenient for describing how light behaves. Light rays are Light rays are convenient for convenient for describing how describing how light behaves. light behaves.
  • 11. Light Rays and Shadows Light Rays and Shadows A geometric analysis may be made of shadows A geometric analysis may be made of shadows by tracing light rays from a point light source: by tracing light rays from a point light source: shadow shadow screen screen Point Point source source The dimensions of the shadow can be found by using geometry and known distances. The dimensions of the shadow can be found by using geometry and known distances.
  • 12. Example 2: Example 2: The diameter of the ball is The diameter of the ball is 4 cm 4 cm and it is located and it is located 20 cm 20 cm from the point light from the point light source. If the screen is source. If the screen is 80 cm 80 cm from the from the source, what is the diameter of the shadow? source, what is the diameter of the shadow? 4 cm 20 cm 80 cm h The ratio of shadow to the source is same as that of ball to source. Therefore: The ratio of The ratio of shadow to shadow to the source the source is same as is same as that of ball that of ball to source. to source. Therefore: Therefore: (4 cm)(80 cm) 20 cm h  h = 16 cm 4 cm 80 cm 20 cm h 
  • 13. Shadows of Extended Objects Shadows of Extended Objects Extended Extended source source penumbra penumbra umbra umbra The The umbra umbra is the region where no light reaches is the region where no light reaches the screen. the screen. • • The The penumbra penumbra is the outer area where is the outer area where only part of the light reaches the screen. only part of the light reaches the screen. • • The The umbra umbra is the region where no light is the region where no light reaches the screen. reaches the screen.
  • 14. The Sensitivity Curve The Sensitivity Curve Sensitivity curve Sensitivity curve Wavelength Wavelength   Sensitivity Sensitivity Human eyes are not Human eyes are not equally sensitive to equally sensitive to all colors. all colors. Eyes are most Eyes are most sensi sensi- - tive tive in the mid in the mid- -range range near near  = 555 nm = 555 nm. . 555 nm 555 nm 400 nm 400 nm 700 nm 700 nm 40 W 40 W 40 W 40 W Yellow light appears brighter to the eye than does red light. Yellow Yellow light appears brighter light appears brighter to the eye than does to the eye than does red red light. light.
  • 15. Luminous Flux Luminous Flux Luminous flux Luminous flux is the portion of total radiant power is the portion of total radiant power that is capable of affecting the sense of sight. that is capable of affecting the sense of sight. Typically only about 10% Typically only about 10% of the power (flux) emitted of the power (flux) emitted from a light bulb falls in from a light bulb falls in the visible region. the visible region. The unit for luminous flux is the The unit for luminous flux is the lumen lumen which which will be given a quantitative definition later. will be given a quantitative definition later.
  • 16. A Solid Angle: Steradians A Solid Angle: Steradians Working with luminous flux requires the use of a solid angle measure called the steradian (sr). Working with luminous flux requires the use of a solid angle measure called the steradian (sr).  A R The Steradian 2 A R   A solid angle of one steradian (1 sr) is subtended at the center of a sphere by an area A equal to the square of its radius ( R2 ). A solid angle of one A solid angle of one steradian steradian ( (1 1 sr sr) is ) is subtended at the subtended at the center of a sphere center of a sphere by an area by an area A A equal equal to the square of its to the square of its radius ( radius ( R R2 2 ). ).
  • 17. Example 3. Example 3. What solid angle is subtended at What solid angle is subtended at the center of a sphere by an area of the center of a sphere by an area of 1.6 m 1.6 m2 2? ? The radius of the sphere is The radius of the sphere is 5 m 5 m. .  A 1.6 m2 R 5 m The Steradian 2 A R   2 2 1.60 m (5.00 m)   2 A R    = 0.00640 sr  = 0.00640 sr
  • 18. The Lumen as a Unit of Flux The Lumen as a Unit of Flux One One lumen lumen (lm) (lm) is the is the luminous flux luminous flux emitted from emitted from a a 1/60 cm 1/60 cm2 2 opening in a standard source and opening in a standard source and included in a solid angle of included in a solid angle of one steradian one steradian (1 (1 sr sr). ). In practice, sources of light are usually rated In practice, sources of light are usually rated by comparison to a commercially prepared by comparison to a commercially prepared standard light source. standard light source. A typical A typical 100 100- -W W incandescent incandescent light bulb emits a total radiant light bulb emits a total radiant power of about power of about 1750 lm 1750 lm. This is . This is for light emitted in all directions. for light emitted in all directions.
  • 19. The Lumen in Power Units The Lumen in Power Units Recalling that luminous flux is really radiant Recalling that luminous flux is really radiant power allows us to define the lumen as follows: power allows us to define the lumen as follows: One lumen is equal to 1/680 W of yellow- green light of wavelength 555 nm. One lumen is equal to 1/680 W of yellow One lumen is equal to 1/680 W of yellow- - green light of wavelength 555 nm. green light of wavelength 555 nm. Wavelength Wavelength   Sensitivity curve Sensitivity curve A disadvantage of this A disadvantage of this approach is the need to approach is the need to refer to sensitivity curves refer to sensitivity curves to determine the flux for to determine the flux for different colors of light. different colors of light.
  • 20. Luminous Intensity Luminous Intensity The The luminous intensity luminous intensity I I for a light source for a light source is the luminous flux per unit solid angle. is the luminous flux per unit solid angle.   F I   Luminous intensity: F I   Unit is the candela (cd) A source having an intensity of one candela emits a flux of one lumen per steradian. A source having an intensity of one candela emits a flux of one lumen per steradian.
  • 21. Total flux for Isotropic Source Total flux for Isotropic Source   R R 3 m 3 m An isotropic source emits in An isotropic source emits in all all directions; i.e., over a directions; i.e., over a solid angle of solid angle of 4 4  steradians steradians. . Total flux: F = 4I Total flux: F = 4I The flux confined to area A is: The flux confined to area A is: F = I A F = I A  = 4 = 4  sr sr Thus, for such Thus, for such a source, the a source, the intensity is: intensity is: 4 F F I    
  • 22. Example 4. Example 4. A A 30 30 cd cd spotlight is located spotlight is located 3 m 3 m above a table. The beam is focused on a surface above a table. The beam is focused on a surface area of area of 0.4 m 0.4 m2 2. Find the intensity of the beam. . Find the intensity of the beam. Total flux: F = 4I Total flux: F = 4I F FT T = 4 = 4 (30 (30 cd cd) = 377 lm ) = 377 lm   R R 3 m 3 m The luminous intensity of The luminous intensity of the beam depends on the beam depends on   2 2 2 0.4 m ; 0.0444 sr (3 m) A R      754 lm 0.0444 sr F I    Beam Intensity: Beam Intensity: I = 8490 cd I = 8490 cd
  • 23. Illumination of a Surface Illumination of a Surface The illumination E of a surface A is defined as the luminous flux per unit area (F/A) in lumens per square meter which is renamed a lux (lx). The The illumination illumination E E of a surface of a surface A A is defined as is defined as the luminous flux per unit area ( the luminous flux per unit area (F/A F/A) in ) in lumens lumens per square meter per square meter which is renamed a which is renamed a lux lux (lx) (lx). . Unit: lux (lx) F E A  An illumination of one lux occurs when a flux of one lumen falls on an area of one square meter. An illumination of one lux occurs when a flux of one lumen falls on an area of one square meter.   R R Area Area A A Illumination, Illumination, E E
  • 24. Illumination Based on Intensity Illumination Based on Intensity  R Area A ; ; F F E I F I A      2 but so that I A E A R     2 Illumination, I E R  This equation applies for perpendicular surfaces. The illumination E of a surface is directly proportional to the intensity I and inversely proportional to the square of the distance R. The The illumination illumination E E of a surface is directly of a surface is directly proportional to the proportional to the intensity intensity I I and inversely and inversely proportional to the proportional to the square square of the of the distance R distance R. .
  • 25. Example 5. Example 5. A A 400 400- -cd cd light is located light is located 2.4 m 2.4 m from a tabletop of area from a tabletop of area 1.2 m 1.2 m2 2. What is the . What is the illumination and what flux illumination and what flux F F falls on the table? falls on the table?  R 2 2 400 cd (2.40 m) I E R   E = 69.4 lx Illumination: Illumination: Now, recalling that Now, recalling that E = F/A E = F/A, we find , we find F F from: from: F = EA = F = EA = (69.4 lx)(1.20 m (69.4 lx)(1.20 m2 2) ) F = 93.3 lm
  • 26. The Inverse Square Relationship The Inverse Square Relationship 2 I E R  E/9 E/4 E 3 m 2 m 1 m 1 m2 4 m2 9 m2 If the intensity is 36 lx at 1 m, it will be 9 lx at 2 m and only 4 lx at 3 m.
  • 27. Summary Summary Light may be defined as electromagnetic radiation that is capable of affecting the sense of sight. Light Light may be defined as electromagnetic radiation may be defined as electromagnetic radiation that is capable of affecting the sense of sight. that is capable of affecting the sense of sight. • Rectilinear propagation • Reflection • Refraction c = fc = 3 x 108 m/s c = fc = 3 x 108 m/s General Properties of Light: Red, Red,   700 nm 700 nm Violet, Violet,   400 nm 400 nm
  • 28. Summary (Continued) Summary (Continued) Luminous flux Luminous flux is the portion of total radiant power is the portion of total radiant power that is capable of affecting the sense of sight. that is capable of affecting the sense of sight. Extended Extended source source penumbra penumbra umbra umbra The formation of shadows: The formation of shadows:
  • 29. Summary (Continued) Summary (Continued) Unit: lux (lx) F E A  Total flux: F = 4I Total flux: F = 4I Luminous intensity: F I   Unit is the candela (cd)  A R The Steradian 2 A R  
  • 30. Summary (Cont.) Summary (Cont.)   R R Area Area A A Illumination, Illumination, E E 2 Illumination, I E R  E/9 E/4 E 3 m 2 m 1 m 1 m2 4 m2 9 m2
  • 31. CONCLUSION: Chapter 33 CONCLUSION: Chapter 33 Light and Illumination Light and Illumination