Download - AKAM CE59700 CH3 AKAM - Purdue University
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CE 59700: Digital Photogrammetric Systems Ayman F. Habib1
Chapters 1 & 2• Chapter 1: Photogrammetry
– Definitions and applications– Conceptual basis of photogrammetric processing
• Transition from two-dimensional imagery to three-dimensional information– Automation
• Chapter 2: Electromagnetic radiation– Terminology– Blackbody radiation– Active versus passive remote sensing systems– Wavebands of the electromagnetic radiation
1
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CE 59700: Digital Photogrammetric Systems Ayman F. Habib2
CE59700: Chapter 3
Basic Optics
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CE 59700: Digital Photogrammetric Systems Ayman F. Habib3
Overview• Introduction & objectives• Basic camera components• Reflection and refraction• Lens system: Definitions• Lens equation, aberrations, and distortions• Diffraction• Resolving power of imaging systems
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CE 59700: Digital Photogrammetric Systems Ayman F. Habib4
Photo. Input: Image Coordinate Measurements
4
Flight Direction
xaya
a
x
z
yPerspective Center
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CE 59700: Digital Photogrammetric Systems Ayman F. Habib5
Photo. Input: Image Coordinate Measurements
5
x
y
x
y
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CE 59700: Digital Photogrammetric Systems Ayman F. Habib6
Photogrammetric Output: Ground Coordinates
X
Z
Y
AXA
YA
ZA
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CE 59700: Digital Photogrammetric Systems Ayman F. Habib7
Photogrammetric Mathematical Model
X
Z
Y
AXA
YA
ZA
.........),,,(.........),,,(
AAAya
AAAxa
ZYXfyZYXfx
==
xaya
a
x
z
yPerspective Center
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CE 59700: Digital Photogrammetric Systems Ayman F. Habib8
Objectives• Investigate various factors that might affect:
– Our ability to precisely identify features of interest in the acquired imagery
• Aberrations• Diffraction• Depth of field• Depth of focus• Motion blur
– The accuracy with which we measure the image coordinates of these features
• Distortions (radial and de-centering lens distortions)
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CE 59700: Digital Photogrammetric Systems Ayman F. Habib9
Aberrations
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CE 59700: Digital Photogrammetric Systems Ayman F. Habib10
Distortions
Without distortions With distortions
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CE 59700: Digital Photogrammetric Systems Ayman F. Habib11
Distortions
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CE 59700: Digital Photogrammetric Systems Ayman F. Habib12
Before Distortion Removal
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CE 59700: Digital Photogrammetric Systems Ayman F. Habib13
After Distortion Removal
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CE 59700: Digital Photogrammetric Systems Ayman F. Habib14
Photogrammetric Cameras
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CE 59700: Digital Photogrammetric Systems Ayman F. Habib15
Analog Photogrammetric Cameras
http://cmapspublic.ihmc.us
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CE 59700: Digital Photogrammetric Systems Ayman F. Habib16
Analog Aerial Camera: RC30
http://www.leica-geosystems.com
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CE 59700: Digital Photogrammetric Systems Ayman F. Habib17
Digital Cameras
Block Diagram of a Digital Camera
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CE 59700: Digital Photogrammetric Systems Ayman F. Habib18
Digital Aerial Camera: DMCTM
http://www.ziimaging.com
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CE 59700: Digital Photogrammetric Systems Ayman F. Habib19
Basic Components of a Camera• Lens: collects light and brings it to focus at the image plane• Aperture: opening that controls the amount of light entering
the camera• Shutter: determines the time period during which the
film/digital sensor will be exposed to light• Film/digital sensor: light-sensitive media• Body: light proof housing of the camera mechanism
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CE 59700: Digital Photogrammetric Systems Ayman F. Habib20
Basic Optics• Optics is the science of controlling and manipulating light.• Optics is divided into two main branches:
– Geometric optics, and– Physical optics.
• In geometric optics, light is considered as groups or bundles of rays traveling in straight lines. – These groups or bundles might be parallel to each other, converge
toward each other, or diverge from one another.– If all the rays are traveling parallel to each other, the light is said to
be collimated.
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CE 59700: Digital Photogrammetric Systems Ayman F. Habib21
Basic Optics: Physical Optics• In physical optics, light is treated as a group of
electromagnetic waves in which the light propagation is considered as a progression of these waves.
• Each of these waves has its own amplitude, frequency, and phase.
• If the waves propagate along parallel lines, the light is said to be collimated.
• If the waves propagate along converging or diverging lines, the light is considered to be convergent or divergent, respectively.
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CE 59700: Digital Photogrammetric Systems Ayman F. Habib22
Reflection & Refraction• When a light ray strikes the surface of an object:
– Part of the light may be transmitted through the object material, – Part of it may be reflected, and – Part of it may be absorbed.
• Light passing from one transparent material to another of different composition, as from air to glass, will undergo a change in velocity.
• The velocity in each medium depends on the refractive index of that medium.
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CE 59700: Digital Photogrammetric Systems Ayman F. Habib23
Reflection & Refraction• The refractive index of a medium (n) is defined as:
– n = c/v– where:
• c is the velocity of light in vacuum (3 * 108 m/sec).• v is the velocity of light in the medium under consideration.
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CE 59700: Digital Photogrammetric Systems Ayman F. Habib24
Medium I
Medium II
B
B`
B``
B```
Angle of incidence, i Angle of reflection, r
Angle of refraction, R
Surface Normal
Reflection & Refraction
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CE 59700: Digital Photogrammetric Systems Ayman F. Habib25
Law of reflection• The reflection law controls the path (BB`B``).• The reflection law states that:
– The incident ray, the surface normal, and the reflected ray lie in the same plane.
– The incident angle (i) = the reflection angle (r)
B
B`
B``i r
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CE 59700: Digital Photogrammetric Systems Ayman F. Habib26
Law of Refraction (Snell’s Law)• The refraction law controls the path (BB`B```).• Snell’s Law states that:
– The incident ray, the surface normal, and the refracted ray lie in one plane.
– ni sin(i) = nR sin(R)– where:
• ni is the refractive index of the medium containing the incident ray.
• nR is the refractive index of the medium containing the refracted ray.
26
B
B`
B```
i
R
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CE 59700: Digital Photogrammetric Systems Ayman F. Habib27
Reflection and Refraction: Special Case
Medium I
Medium II
A
A`
A``
A```
• If a light ray is directed from one transparent medium to another normal to the surface separating the two media, part of it will be reflected back on itself.
• The other part continues in the same direction in the second medium.
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CE 59700: Digital Photogrammetric Systems Ayman F. Habib28
Reflection & Refraction• Examining Snell’s Law, we can see that the refracted ray
will be bent toward the surface normal if this medium has higher refractive index.
• If the light ray is directed from a medium of higher refractive index to one of lower refractive index, the ray will be bent away from the surface normal in the second medium. – As the incidence angle increases, the refraction angle also
increases with a greater rate until it reaches (90°).– Beyond this point, the ray is totally reflected.
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CE 59700: Digital Photogrammetric Systems Ayman F. Habib29
Critical Angle• The incident angle, ic, which causes a (90°) angle of
refraction is called the critical angle for the two media. • This angle can be determined from the law of refraction as
follows:
i
Rc n
ni =)sin(
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CE 59700: Digital Photogrammetric Systems Ayman F. Habib30
Lens System• The function of a lens in photogrammetry is to gather light
rays and bring them into focus at a point.• A positive lens changes a divergent light bundle, originating
from a point source, to a convergent bundle. • A negative lens makes the bundle more divergent.
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CE 59700: Digital Photogrammetric Systems Ayman F. Habib31
Lens System
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CE 59700: Digital Photogrammetric Systems Ayman F. Habib32
Basic Definitions
x f f' x's s'
L
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y
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CE 59700: Digital Photogrammetric Systems Ayman F. Habib33
Basic Definitions• Optical System:
– any device that operates on light to produce a specific and desired effect
• Optical Axis: – the rotational axis of the optical system that passes through the centers of
curvature of surfaces comprising the lens system
• Principal Planes (H, H`): – are perpendicular to the optical axis and located in such a way that the lateral
magnification at their location is unity and positive
• Lateral Magnification:– the ratio between the image and object size
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CE 59700: Digital Photogrammetric Systems Ayman F. Habib34
Basic Definitions• Nodal Points (N, N`):
– are the intersection of the principal planes with the optical axis.– a ray passing through the first nodal point will emerge from the rear nodal point
parallel to the incident ray.
• Focal Points (F, F`):– are the axial points where the images of axial objects at infinity are located.
• Focal Length (f, f`):– is the distance between the focal point and the corresponding nodal point.
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CE 59700: Digital Photogrammetric Systems Ayman F. Habib35
Lens Equation• The lens equation relates the focal length (f`), the image
distance (s`), and the object distance (s).– 1/f` = 1/s + 1/s`
• Notes:– When s → ∞ then s` → f`– A ray parallel to the optical axis will be refracted in such a way
that it passes through the rear focal point.– A ray through the front nodal point will emerge from the rear
nodal point without changing its direction.– These simple rules allow for graphic construction of images.– From now on, we will assume that f is equal to f`.
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CE 59700: Digital Photogrammetric Systems Ayman F. Habib36
Image Formation from Geometric Optics
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CE 59700: Digital Photogrammetric Systems Ayman F. Habib37
Lens Equation for Aerial Cameras• The object distance (s) is defined by the flying height above
the ground (H - h).• The image distance (s`) is usually labeled as the camera
constant or principal distance (c).• The object distance (s) is very large when compared to the
focal length (f).– s ≈ ∞– Therefore, the image distance (s`) is set to the focal length (f).– c = f
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CE 59700: Digital Photogrammetric Systems Ayman F. Habib38
Paraxial Region• Assumptions made in geometric optics for image formation
lead to inaccuracies, which are proportional to the angle between a light ray and the optical axis (off-axial angle).
• The lens formula is only valid for very small off-axial angles where:– Sin (θ) = θ in radians, and – tan (θ) = θ in radians.
• That is, it is only valid for objects close to the optical axis. – This area is called the paraxial region.
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CE 59700: Digital Photogrammetric Systems Ayman F. Habib39
Lens Aberrations• Assumption: An object point will be imaged as a point.• Actually: An object point will be imaged as a blur.• Reason: Lens Aberrations• Factors causing aberrations include:
– Different wavelengths of the incident light,– Object points with large off-axial angle, and– Manufacturing flaws.
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CE 59700: Digital Photogrammetric Systems Ayman F. Habib40
Lens Aberrations• Aberration can be classified according to their origin as
following:– Aberrations caused by large aperture and/or off-axial objects
• Spherical aberration; Astigmatism and Curvature of field; and Coma– Aberrations caused by different wavelengths of the incident light
• Chromatic aberrations– Aberrations caused by manufacturing flaws
• Irregular aberrations
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CE 59700: Digital Photogrammetric Systems Ayman F. Habib41
Aberrations Due to Axial and Off-Axial Objects
Position of object point Small aperture angle(Narrow Bundle)
Large aperture angle(Wide Bundle)
Axial Aberration free Spherical aberration
Off-Axial Astigmatism and curvature of field Coma
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CE 59700: Digital Photogrammetric Systems Ayman F. Habib42
Marginal Ray
F′
Longitudinal spherical aberration
h
Spherical Aberrations
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CE 59700: Digital Photogrammetric Systems Ayman F. Habib43
Spherical Aberrations• Spherical aberration applies only to points lying on the
optical axis. • Regardless where the image plane is located, the resulting
image of a point will be a small circle. • The longitudinal spherical aberration depends on the height
(h).– The distance between the marginal rays and optical axis (radius of
the aperture)• The best image quality is reached at a position between the
foci of the marginal rays and the paraxial rays. – The cross section of the bundle of rays at this location is known as
the circle of least confusion.
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CE 59700: Digital Photogrammetric Systems Ayman F. Habib44
Spherical Aberrations• The longitudinal aberration is proportional to h2.• The radius of the circle of least confusion is proportional to
h3.• Consequently, stopping down the lens (i.e., reducing the
diameter of the aperture) decreases the effect of spherical aberrations.
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CE 59700: Digital Photogrammetric Systems Ayman F. Habib45
TSC
F’
Image plane for axial points
Astigmatism and Curvature of Field
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CE 59700: Digital Photogrammetric Systems Ayman F. Habib46
Astigmatism and Curvature of Field• A narrow but oblique bundle intercepts the lens surface
non-symmetrically. • As a result, the bundle in the image space does not precisely
intersect in one point but in two short lines.• The separation (longitudinal distance) between these lines is
called astigmatism and curvature of field.
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CE 59700: Digital Photogrammetric Systems Ayman F. Habib47
Coma
F’
Focal plane
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CE 59700: Digital Photogrammetric Systems Ayman F. Habib48
Coma• The image of an off-axial object with a wide bundle has a
comet-shape blur. • Like astigmatism, coma is the result of the non-symmetric
intercept of the oblique and wide bundle with the lens.
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CE 59700: Digital Photogrammetric Systems Ayman F. Habib49
Chromatic Aberrations• Chromatic aberration is caused by the fact that glass has
different refractive indices for different wavelengths. • As a result, every wavelength has its separate focus.• This is a similar situation to the case of spherical aberration.
http://en.wikipedia.org/wiki/Chromostereopsis
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CE 59700: Digital Photogrammetric Systems Ayman F. Habib50
Chromatic Aberrations
Image captured with a high quality lens
Image captured with a lens showing chromatic aberrations
http://en.wikipedia.org/wiki/Chromostereopsis
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CE 59700: Digital Photogrammetric Systems Ayman F. Habib51
Diffraction• Diffraction is caused by the interference of light waves with
the aperture.• As a result, an object point will appear as a small disc
surrounded by a number of dark and bright rings.• The radius of the central disc (r) can be computed as
follows:– r = 1.22 λ (f/d) where:
λ is the wavelength of the light,f is the focal length, andd is the diameter of the aperture.
51
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CE 59700: Digital Photogrammetric Systems Ayman F. Habib52
Diffraction
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CE 59700: Digital Photogrammetric Systems Ayman F. Habib53
Diffraction• If two discs are to be moved towards each other, a point will
be reached at which the two discs will no longer be identified as two separate objects.
• This is the case when the two objects are separated by the radius of one disc.
• The reciprocal of the disc radius is a measure of the resolving power of the lens system (optical resolution).
mmlinesdf
r /)/(22.1
1/1ResolutionOpticalλ
==
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CE 59700: Digital Photogrammetric Systems Ayman F. Habib54
Diffraction
r
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CE 59700: Digital Photogrammetric Systems Ayman F. Habib55
Resolving Power of an Imaging system• Resolution is the ability of the system to identify nearby
objects as separate entities.• We want to establish a quantitative measure of the
capability of our imaging system (camera and film) to image neighboring points or lines as separate entities.
• The resolution is measured in line-pairs per mm using resolution test chart.
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CE 59700: Digital Photogrammetric Systems Ayman F. Habib56
Resolution Test Chart
http://www.dennishollingsworth.us/archives/image/test-pattern-1-TVE.gif
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CE 59700: Digital Photogrammetric Systems Ayman F. Habib57
Resolving Power of an Imaging system• Factors that affect the resolving power include:
– Lens aberrations,– Depth of field,– Depth of focus,– Diffraction,– Film material or CCD/CMOS array, and– Motion blur.
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CE 59700: Digital Photogrammetric Systems Ayman F. Habib58
Depth of Field
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CE 59700: Digital Photogrammetric Systems Ayman F. Habib59
AF
A
AN
A
pA qA
Depth of field Image plane forobject point A
aN
a
af
c
c
Circle of confusionsame size at bothapertures
Depth of Field• The distance in the object space within which the object
point can be moved and still be in acceptable focus.
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CE 59700: Digital Photogrammetric Systems Ayman F. Habib60
Depth of Focus
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CE 59700: Digital Photogrammetric Systems Ayman F. Habib61
Depth of Focus• Depth of focus is the distance in front or behind the plane of
best focus for a given object distance where the image is still in acceptable focus.
Image plane
Circle of confusion same size at both apertures
Image plane
d d
d d
p q
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CE 59700: Digital Photogrammetric Systems Ayman F. Habib62
Factors Affecting Depth of Field/Depth of Focus• The focal length• The object distance• The diameter of the aperture stop
– The smaller the aperture the larger the depth of field and focus.• The radius of the acceptable circle of confusion
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CE 59700: Digital Photogrammetric Systems Ayman F. Habib63
Motion Blur• During the exposure of the photograph, the camera shutter
remains open for a short time (dt) while the aircraft is still flying at a velocity (V).– This causes a blur (motion blur) in the captured image.
• The magnitude of the motion blur depends on:– The shutter opening time/shutter speed (dt),– The velocity of the aircraft (V),– The flying height (h), and– The camera constant – principal distance (c).
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CE 59700: Digital Photogrammetric Systems Ayman F. Habib64
Motion Blur
A
a1
o1
a1
o2
a2a2
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CE 59700: Digital Photogrammetric Systems Ayman F. Habib65
dr / c = V * dt / hdr = V * dt * c / h
OO`
A
V dt
dr
c
h
a a`
Motion Blur
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CE 59700: Digital Photogrammetric Systems Ayman F. Habib66
Motion Blur• To avoid motion blur, some photogrammetric cameras have
a mechanism that causes the film to advance forward in the flight direction during the exposure time.
• The advancement magnitude should be exactly (dr).• This advancement is known as the image motion
compensation.
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CE 59700: Digital Photogrammetric Systems Ayman F. Habib67
Distortion
Distortion
Incident Light Ray
a`
Theoretical Light Ray
a
Actual Light Ray
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CE 59700: Digital Photogrammetric Systems Ayman F. Habib68
Distortion• Definition: Image points are displaced from their theoretical
location.
• Aberrations will affect the precision of the final image coordinate measurements.
• Distortions will affect the accuracy of the final image coordinate measurements.
Theoretical Light Ray Actual Light Ray
Distortion
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CE 59700: Digital Photogrammetric Systems Ayman F. Habib69
Radial Lens Distortion• The light ray changes its direction after passing through the
perspective center.• Radial lens distortion is caused by:
– Large off-axial angle, and– Lens manufacturing flaws.
• Radial lens distortion occurs along a radial direction from the center of the image.
• Radial lens distortion increases as we move away from the optical axis.
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Radial Lens Distortion
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CE 59700: Digital Photogrammetric Systems Ayman F. Habib71
Without distortions With distortions
Radial Lens Distortion
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CE 59700: Digital Photogrammetric Systems Ayman F. Habib72
Pin Cushion Type Radial Lens Distortion
Radial Lens Distortion
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CE 59700: Digital Photogrammetric Systems Ayman F. Habib73
Radial Lens Distortion
Barrel Type Radial Lens Distortion
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Before Distortion Removal
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After Distortion Removal
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Lens Cone Assembly
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http://static.trustedreviews.com/94/44ca5a/dec1/4778-KonMinA2.jpg
Lens Cone Assembly
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De-centering Lens Distortion
Theoretical Optical Axis
Actual Optical Axis
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CE 59700: Digital Photogrammetric Systems Ayman F. Habib79
De-centering Lens Distortion• De-centering lens distortion is caused by miss alignment of
the components of the lens system.• De-centering lens distortion has two components:
– Radial component, and– Tangential component.
79
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De-centering Lens Distortion
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Without distortions With distortions
De-centering Lens Distortion
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CE 59700: Digital Photogrammetric Systems Ayman F. Habib82
Summary• In this chapter, we covered the following topics:
– Basics of geometric optics– Factors affecting the precision of the final image coordinate
measurements:• Aberrations, diffraction, depth of field, depth of focus, and motion blur• Resolving power of the imaging system
– Factors affecting the accuracy of the final image coordinate measurements:
• Radial and de-centering lens distortion