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nate system W into the camera coordinate system C i . The transformation C W T is
composed of a rotational part R i , corresponding to an orthonormal matrix of size
3
3 determined by three independent parameters, e.g. the Euler rotation angles
(Craig, 1989 ), and a translation vector t i denoting the offset between the coordinate
systems. This decomposition yields
C i x
×
W T W x = R i W x
C i
=
+
t i .
(1.2)
Furthermore, the image formation process is determined by the intrinsic parameters
{
c j } i of each camera i , some of which are lens-specific while others are sensor-
specific. For a camera described by the pinhole model and equipped with a digital
sensor, these parameters comprise the principal distance b , the effective number of
pixels per unit length k u and k v along the horizontal and the vertical image axes,
respectively, the pixel skew angle θ , and the coordinates u 0 and v 0 of the prin-
cipal point in the image plane (Birchfield, 1998 ). For most modern camera sen-
sors, the skew angle amounts to θ
90
=
and the pixels are of quadratic shape with
k u =
k v .
For a real lens system, however, the observed image coordinates of scene points
may deviate from those given by ( 1.1 ) due to the effect of lens distortion. In this
work we employ the lens distortion model by Brown ( 1966 , 1971 ) which has been
extended by Heikkilä and Silvén ( 1997 ) and by Bouguet ( 1999 ). According to
Heikkilä and Silvén ( 1997 ), the distorted coordinates I x d of a point in the image
plane are obtained from the undistorted coordinates I x by
I x d = 1
k 5 r 6 I x
k 1 r 2
k 3 r 4
+
+
+
+
d t ,
(1.3)
where I x
v 2 . If radial distortion is present, straight lines in
the object space crossing the optical axis still appear straight in the image, but the
observed distance of a point in the image from the principal point deviates from the
distance expected according to ( 1.1 ). The vector
v) T
and r 2
u 2
=
(
u,
ˆ
ˆ
2 k 2 ˆ
k 4 (r 2
u 2 )
u
v
ˆ
+
+
2
ˆ
d t =
(1.4)
k 2 (r 2
v 2 )
+
2
ˆ
+
2 k 4 ˆ
u
v
ˆ
is termed tangential distortion. The occurrence of tangential distortion implies that
straight lines in the object space crossing the optical axis appear bent in some direc-
tions in the image.
When a film is used as an imaging sensor,
v directly denote metric dis-
tances on the film with respect to the principal point, which has to be determined by
an appropriate calibration procedure (cf. Sect. 1.4 ). When a digital camera sensor is
used, the transformation
u and
ˆ
ˆ
I T I x
S x
S
=
(1.5)
from the image coordinate system into the sensor coordinate system is defined in the
general case by an affine transformation
S
I T (as long as the sensor has no 'exotic'
architecture such as a hexagonal pixel raster, where the transformation would be
still more complex). The corresponding coordinates
S x
(u, v) T
=
are measured in
pixels.
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