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GE 178 Lecture 6:
Distortion and Displacement
Relief Displacement
Tilt Displacement
DISTORTION VS. DISPLACEMENT
Distortion shift in the location of an object, which
changes the perspective characteristics of
the photo
Types of Distortion
1. Film and Print Shrinkage – negligible effect*
2. Atmospheric Refraction of Light Rays – negligible effect*
3. Image Motion
4. Lens Distortion
*Except for precise mapping projects
Lens Distortion
small effects due to the flaws in the optical components (lens) of camera systems leading to distortions
typically more serious at the edges of photo
radial from the principal point
makes objects appear either closer to, or farther from the principal point than they actually are
may be corrected using calibration curves
examples: car windows/windshields, carnival mirrors
Lens Distortion
Lens Distortion
Displacement
shift in the location of an object in a photo,
which does not change the perspective
characteristics of the photo
fiducial distance between an object's image and
it's true plan position, caused by change in
elevation
Types of Displacement
1. Curvature of the Earth – negligible effect*
2. Relief Displacement – radial from the nadir
3. Tilt Displacement – radial from the isocenter
*Except for precise mapping projects
Major Causes of Non-uniformity in
Scale within a Single Photograph 1. Relief Displacement
2. Tilt Displacement
Relief
Displacement
Relief Displacement
Error in the position of the point in a photograph because of relief
The position of a point in the photograph (which has a central projection) is different from its corresponding position on the map (which has an orthogonal projection) due to relief
Radial from the nadir (assuming a vertical photograph, therefore, nadir = center of photo)
Relief Displacement
Relief Displacement
The farther a point is from the nadir, the greater the
displacement
Relief Displacement
Relief Displacement
Relief Displacement
f
Hmge (flying height)
datum plane
∆h
r’
∆r
CASE 1:
Point is above the datum plane
datum plane
Relief Displacement
f
Hmge (flying height)
∆h
r’
∆r
CASE 2:
Point is below the datum plane
Relief Displacement
r'
a‘ a
A’
A
Class
Exercise: Derive the
equation for relief
displacement Dr
Dr
Formula for Relief Displacement
Where:
r’ = erroneous radial distance from the center of photo
h = height/elevation of the point above/below the datum
plane
H = flying height above the datum plane
H
hrr
'D
General Conclusion: Elevation and Relief Displacement
The higher the point is above the datum plane
(or the lower it is below the datum plane), the
greater the relief displacement
The higher the flying height, the lesser the
relief displacement
H
hrr
'D
Corrected Radial Distance
If the point on the ground is ABOVE the datum,
the corrected position will be towards the center
Otherwise, if the point is BELOW the datum, the
corrected position will be away from the center
'r r r D
'r r r D
Occlusion
Occlusion
How can we minimize ∆r?
Use only the central part of the photograph
(discard the edges)
Fly higher but this would yield a smaller
photoscale
Fly higher, and use a camera with a larger focal
length (for example, use a normal angle camera
instead of a wide-angle camera)
H
hrr
'D
Example
A 1:15000 aerial photograph was taken using a
wide-angle camera. A point on the photograph
was identified and its measured distance from the
center is 5.4 centimeters. If the corresponding
point on the ground is elevated from the datum by
60 meters, determine the displacement due to
relief and the correct radial distance of the point
from the center of the photo.
Solution
6 inches
16*2.54*1 100
15000
2286 meters
' (0.054)(60)
2286
0.001417322 meters
0.1417322 cms.
f
H
H
r hr
H
r
r
DD
D
D
'
5.4 0.1417322
5.2582678 cms.
r r r
r
r
D
Quiz 1 (1/4 Sheet of paper)
The top and bottom of a utility pole in an
image are 129.8 mm and 125.2 mm,
respectively, from the principal point of a
vertical photograph. What is the height of the
pole if the flying height above the base of the
pole is 875m?
Tilt
Displacement
b’’
n
p
i
t
a’
a’’
b’
Tilt Displacement
An error in the position of a point on the
photograph due to indeliberate tilting of the aircraft
Due to instability of aircraft
May be due to tilting of the aircraft along the flight
line and/or perpendicular to the flight line
Increases radially from the isocenter
∆ta
b’’
Tilt Displacement
n
p
i
t
a’
a’’
ya
yb
b’
∆tb
Principal Line Line of maximum tilt
Line connecting the principal point, isocenter and nadir
All lines perpendicular to this line are lines of zero inclination
or zero phototilt
this means that all points along a perpendicular line
have uniform scale
∆ta
b’’
Tilt
Displacement
n
p
i
t
a’
a’’
ya
yb
b’
∆tb
Phototilt (t)
Amount of tilt of the aircraft
(and thus the camera lens)
with respect to the vertical
axis
Angle of tilt between the line
perpendicular to the horizontal
datum and the line
perpendicular to the lens
Formula for Phototilt
Where:
t = phototilt
Sa = scale of first point, projected to the principal line
Sb = scale of second point, projected to the principal line
y = distance between a and b along the principal line
Hmge = flying height with respect to the mean ground
sin b amge mge
S SdSt H H
y y
Locating the Nadir and Isocenter
Nadir – radial center of relief displacement
Isocenter – radial center of tilt displacement
distance between p and n (pn) tan
distance between p and i (pi) tan2
f t
tf
Formula for Tilt Displacement
Formula for Tilt Displacement
Where:
i = isocenter
y = projection of erroneous radial distance from the isocenter (i) to the point along the principal line
f = focal length
t = phototilt
2 sin
sin
y tt
f y tD
Corrected Radial Distance
if the point on the ground is above the horizontal 'r r t D
'r r t D if the point on the ground
is below the horizontal
Auxiliary Tilted Photo Coordinate System
'sincos
fy t
tSH h
Scale of a Tilted Photograph
Tilt Displacement Practical Solution PROBLEM:
may cause large errors in determining scale and
distances
SOLUTION:
use 2 known or measurable ground distances that are:
About the same elevation
Equal distances from the photo center
Diametrically opposite from the center
END OF LECTURE