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FUNDAMENTALS OF IMAGING
CS-467 Digital Image Processing
1
Some features of vision
• The innermost membrane of the eye is the
retina
• Pattern vision is afforded by the distribution of
discrete light receptors over the surface of the
retina
• There are two classes of receptors: cones and
rods
2
Some Features of Vision
• Cones (there are about 6-7 million cones in
each eye) are highly sensitive to color. Each
cone is connected to its own nerve end.
• Rods (there are about 75-150 million rods in
each eye) are responsible for creation of a
general, overall picture of the field of view.
Rods are not sensitive to color and several of
them are connected to a single nerve end.
3
Image Formation in the Eye
4
15 17 15
100 17 100
h
h
×
= ⇒ = h= height of the image created in the eye
© 1992-2008 R.C. Gonzalez & R.E. Woods
Brightness Adaptation and
Discrimination
• The range of light intensity levels to which the
human visual system can adapt is on the order
of 1010
• However, our visual system is unable to
percept so many intensity levels at a time. It
can adapt itself to a small sub-range, which is
determined by a logarithmic function of the
light intensity
5
Brightness Adaptation and
Discrimination
• Short curves show ranges of intensity to which
human visual system has adapted
6
© 1992-2008 R.C. Gonzalez & R.E. Woods
Light and Electromagnetic Spectrum
7
c
v
λ =
E hv=
Correspondence between the wavelength and the frequency
The Energy of the component of electromagnetic spectrum
c is the speed of light; h is Planck’s constant
Light and Electromagnetic
Spectrum
• Since energy is proportional to frequency,
then the higher frequency is, the more energy
is carried by the corresponding
electromagnetic phenomenon – the more
energy is per photon there
8
E hv=
Electromagnetic Wave and
Wavelength
• The wavelength of an electromagnetic wave
required to “see” an object, must be of the same
size or smaller than the object
• For example, to see a water molecule (diameter
10-10 m), we would need a source capable of
emitting in the far ultraviolet or soft X-ray region)
9
© 1992-2008 R.C. Gonzalez & R.E. Woods
Monochromatic Light
• Light is a particular type of electromagnetic
radiation (phenomenon) that can be sensed by
the human eye.
• Monochromatic light is void of color. Its intensity
varies from black to white.
• The levels of intensity of monochromatic light are
called gray levels.
• The range of measured values of monochromatic
light from black to white are called gray-scale.
• Monochromatic images are referred to as
gray-scale images.
10
Light Properties
• Radiance (watts – W) is the total amount of
energy that flows from the light source
• Luminance (lumens-lm) is a measure of the
amount of energy an observer perceives from
a light source (for example, in the infrared
region it tends to zero, although the same
light may have significant radiance)
• Brightness is a subjective descriptor of light
perception (it is impossible to measure it)
11
Image Sensing and Acquisition
• Most of digital images are generated by the
combination of an “illumination” (energy)
source and the reflection or absorption of
energy from that source by the elements of
the “scene” being imaged.
12
Image Sensing and Acquisition
13
© 1992-2008 R.C. Gonzalez & R.E. Woods
Single Sensor
Line Sensor
Array Sensor – CCD
( a Charge-Coupled
Device)
Image Sensing and Acquisition
14
A single sensor
© 1992-2008 R.C. Gonzalez & R.E. Woods
Image Sensing and Acquisition
15
© 1992-2008 R.C. Gonzalez & R.E. Woods
Image Formation Model
16
© 1992-2008 R.C. Gonzalez & R.E. Woods
Digital Image
• Mathematically, a digital image can be
considered as a discrete function
• is a finite domain (which is called a spatial
domain) of the image-function, and I is a co-
domain of the image-function
17
( ) { } { }2
, : ; 0,1,2,..., 1 , 0,1,..., 1f x y D I D N I L→ = − = −
2
D
Image Formation Model
• When an image (x and y are spatial
domain coordinates) is generated from a
physical process, its intensity values are
proportional to energy radiated by a physical
source (by electromagnetic waves).
• must be nonzero and finite:
18
( ),f x y
( ),f x y
( )0 ,f x y< < ∞
Image Formation Model
• is characterized by
• (1) the amount of source illumination
incident on the scene being viewed
(illumination)
• (2) the amount of illumination reflected by
(transmitted through for X-ray or γ-ray) the
objects in this scene (reflectance)
19
( ),f x y
( ) ( ) ( )
( )
( )
, , ,
0 ,
0 , 1
f x y i x y r x y
i x y
r x y
=
< < ∞
< <
( ),i x y
( ),r x y
Image Formation Model
• is determined by illumination source
• is determined by characteristics of the
imaged objects
• means total absorption
• means total reflectance (passing
through for X-ray or γ-ray)
20
( ) ( ) ( )
( )
( )
, , ,
0 ,
0 , 1
f x y i x y r x y
i x y
r x y
=
< < ∞
< <
( ),i x y
( ),r x y
( ), 0r x y →
( ), 1r x y →
Image Formation Model
• In any particular case, there are Lmin and Lmax
that limit a range for
• If then always
• In practice,
• The interval is called the gray scale
• Common practice is to shift it to
21
( ),f x y
( )0 0,l f x y= min maxL l L≤ ≤
min min min max max max;L i r L i r= =
[ ]min max,L L
[ ]
max min
min min max min
1; 1
0,, 1
L L L L
L L L L L
=− = − +
 
 − − =
 
 
−

Image Formation Model
• 0 corresponds to black
• L-1 corresponds to white
• We say that the gray scale contains L gray
levels
22
[ ]
max min
min min max min
1; 1
0,, 1
L L L L
L L L L L
=− = − +
 
 − − =
 
 
−

Concepts of Sampling and
Quantization
• Any natural image is continuous with respect
to the x- and y-coordinates, and also in its
amplitude
• Digitizing the coordinate values is called
sampling
• Digitizing the intensity values is called
quantization
23
Concepts of Sampling and
Quantization
24
© 1992-2008 R.C. Gonzalez & R.E. Woods
Concepts of Sampling and
Quantization
25
© 1992-2008 R.C. Gonzalez & R.E. Woods
Sampling Theorem
• Sampling theorem by Nyquist–Shannon–Kotelnikov-
Whittaker (1949) establishes necessary condition for the
ability to reconstruct a signal from its samples.
• Sampling theorem (1-D case, time domain).
A bandlimited analog signal, which has been sampled,
can be perfectly reconstructed from an infinite
sequence of samples if the sampling rate exceeds 2N
samples per second, where N is the highest frequency in
the original signal. If a signal contains a component at
exactly frequency N , then samples spaced at exactly
1/(2N) seconds do not completely determine the signal.
26
Sampling Theorem
• The signal x(t) is said to be bandlimited if for its
Fourier transform
if the following property holds:
27
2
( ) ( ) i t
xF x t e dtπω
ω
∞
−
−∞
= ∫
( ) 0 for | |xF Nω ω= >
Sampling Theorem
• Sampling theorem (2-D case, spatial domain).
A bandlimited analog signal, which has been
sampled, can be perfectly reconstructed from
an infinite sequence of samples if the sampling
rate exceeds 2N samples per unit distance,
where N is the highest frequency in the original
signal. If a signal contains a component at
exactly frequency N , then samples spaced at
exactly 1/(2N) per unit distance do not
completely determine the signal.
28
Spatial Resolution
29
© 1992-2008 R.C. Gonzalez & R.E. Woods
Intensity Resolution
30
© 1992-2008 R.C. Gonzalez & R.E. Woods
Intensity Resolution
31
© 1992-2008 R.C. Gonzalez & R.E. Woods

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Lecture 2

  • 1. FUNDAMENTALS OF IMAGING CS-467 Digital Image Processing 1
  • 2. Some features of vision • The innermost membrane of the eye is the retina • Pattern vision is afforded by the distribution of discrete light receptors over the surface of the retina • There are two classes of receptors: cones and rods 2
  • 3. Some Features of Vision • Cones (there are about 6-7 million cones in each eye) are highly sensitive to color. Each cone is connected to its own nerve end. • Rods (there are about 75-150 million rods in each eye) are responsible for creation of a general, overall picture of the field of view. Rods are not sensitive to color and several of them are connected to a single nerve end. 3
  • 4. Image Formation in the Eye 4 15 17 15 100 17 100 h h × = ⇒ = h= height of the image created in the eye © 1992-2008 R.C. Gonzalez & R.E. Woods
  • 5. Brightness Adaptation and Discrimination • The range of light intensity levels to which the human visual system can adapt is on the order of 1010 • However, our visual system is unable to percept so many intensity levels at a time. It can adapt itself to a small sub-range, which is determined by a logarithmic function of the light intensity 5
  • 6. Brightness Adaptation and Discrimination • Short curves show ranges of intensity to which human visual system has adapted 6 © 1992-2008 R.C. Gonzalez & R.E. Woods
  • 7. Light and Electromagnetic Spectrum 7 c v λ = E hv= Correspondence between the wavelength and the frequency The Energy of the component of electromagnetic spectrum c is the speed of light; h is Planck’s constant
  • 8. Light and Electromagnetic Spectrum • Since energy is proportional to frequency, then the higher frequency is, the more energy is carried by the corresponding electromagnetic phenomenon – the more energy is per photon there 8 E hv=
  • 9. Electromagnetic Wave and Wavelength • The wavelength of an electromagnetic wave required to “see” an object, must be of the same size or smaller than the object • For example, to see a water molecule (diameter 10-10 m), we would need a source capable of emitting in the far ultraviolet or soft X-ray region) 9 © 1992-2008 R.C. Gonzalez & R.E. Woods
  • 10. Monochromatic Light • Light is a particular type of electromagnetic radiation (phenomenon) that can be sensed by the human eye. • Monochromatic light is void of color. Its intensity varies from black to white. • The levels of intensity of monochromatic light are called gray levels. • The range of measured values of monochromatic light from black to white are called gray-scale. • Monochromatic images are referred to as gray-scale images. 10
  • 11. Light Properties • Radiance (watts – W) is the total amount of energy that flows from the light source • Luminance (lumens-lm) is a measure of the amount of energy an observer perceives from a light source (for example, in the infrared region it tends to zero, although the same light may have significant radiance) • Brightness is a subjective descriptor of light perception (it is impossible to measure it) 11
  • 12. Image Sensing and Acquisition • Most of digital images are generated by the combination of an “illumination” (energy) source and the reflection or absorption of energy from that source by the elements of the “scene” being imaged. 12
  • 13. Image Sensing and Acquisition 13 © 1992-2008 R.C. Gonzalez & R.E. Woods Single Sensor Line Sensor Array Sensor – CCD ( a Charge-Coupled Device)
  • 14. Image Sensing and Acquisition 14 A single sensor © 1992-2008 R.C. Gonzalez & R.E. Woods
  • 15. Image Sensing and Acquisition 15 © 1992-2008 R.C. Gonzalez & R.E. Woods
  • 16. Image Formation Model 16 © 1992-2008 R.C. Gonzalez & R.E. Woods
  • 17. Digital Image • Mathematically, a digital image can be considered as a discrete function • is a finite domain (which is called a spatial domain) of the image-function, and I is a co- domain of the image-function 17 ( ) { } { }2 , : ; 0,1,2,..., 1 , 0,1,..., 1f x y D I D N I L→ = − = − 2 D
  • 18. Image Formation Model • When an image (x and y are spatial domain coordinates) is generated from a physical process, its intensity values are proportional to energy radiated by a physical source (by electromagnetic waves). • must be nonzero and finite: 18 ( ),f x y ( ),f x y ( )0 ,f x y< < ∞
  • 19. Image Formation Model • is characterized by • (1) the amount of source illumination incident on the scene being viewed (illumination) • (2) the amount of illumination reflected by (transmitted through for X-ray or γ-ray) the objects in this scene (reflectance) 19 ( ),f x y ( ) ( ) ( ) ( ) ( ) , , , 0 , 0 , 1 f x y i x y r x y i x y r x y = < < ∞ < < ( ),i x y ( ),r x y
  • 20. Image Formation Model • is determined by illumination source • is determined by characteristics of the imaged objects • means total absorption • means total reflectance (passing through for X-ray or γ-ray) 20 ( ) ( ) ( ) ( ) ( ) , , , 0 , 0 , 1 f x y i x y r x y i x y r x y = < < ∞ < < ( ),i x y ( ),r x y ( ), 0r x y → ( ), 1r x y →
  • 21. Image Formation Model • In any particular case, there are Lmin and Lmax that limit a range for • If then always • In practice, • The interval is called the gray scale • Common practice is to shift it to 21 ( ),f x y ( )0 0,l f x y= min maxL l L≤ ≤ min min min max max max;L i r L i r= = [ ]min max,L L [ ] max min min min max min 1; 1 0,, 1 L L L L L L L L L =− = − +    − − =     − 
  • 22. Image Formation Model • 0 corresponds to black • L-1 corresponds to white • We say that the gray scale contains L gray levels 22 [ ] max min min min max min 1; 1 0,, 1 L L L L L L L L L =− = − +    − − =     − 
  • 23. Concepts of Sampling and Quantization • Any natural image is continuous with respect to the x- and y-coordinates, and also in its amplitude • Digitizing the coordinate values is called sampling • Digitizing the intensity values is called quantization 23
  • 24. Concepts of Sampling and Quantization 24 © 1992-2008 R.C. Gonzalez & R.E. Woods
  • 25. Concepts of Sampling and Quantization 25 © 1992-2008 R.C. Gonzalez & R.E. Woods
  • 26. Sampling Theorem • Sampling theorem by Nyquist–Shannon–Kotelnikov- Whittaker (1949) establishes necessary condition for the ability to reconstruct a signal from its samples. • Sampling theorem (1-D case, time domain). A bandlimited analog signal, which has been sampled, can be perfectly reconstructed from an infinite sequence of samples if the sampling rate exceeds 2N samples per second, where N is the highest frequency in the original signal. If a signal contains a component at exactly frequency N , then samples spaced at exactly 1/(2N) seconds do not completely determine the signal. 26
  • 27. Sampling Theorem • The signal x(t) is said to be bandlimited if for its Fourier transform if the following property holds: 27 2 ( ) ( ) i t xF x t e dtπω ω ∞ − −∞ = ∫ ( ) 0 for | |xF Nω ω= >
  • 28. Sampling Theorem • Sampling theorem (2-D case, spatial domain). A bandlimited analog signal, which has been sampled, can be perfectly reconstructed from an infinite sequence of samples if the sampling rate exceeds 2N samples per unit distance, where N is the highest frequency in the original signal. If a signal contains a component at exactly frequency N , then samples spaced at exactly 1/(2N) per unit distance do not completely determine the signal. 28
  • 29. Spatial Resolution 29 © 1992-2008 R.C. Gonzalez & R.E. Woods
  • 30. Intensity Resolution 30 © 1992-2008 R.C. Gonzalez & R.E. Woods
  • 31. Intensity Resolution 31 © 1992-2008 R.C. Gonzalez & R.E. Woods