The International Archives of the Photogrammetry, Remote Sensing and Spatial Information Sciences. Vol. XXXVII. Part Bl. Beijing 2008
291
knowledge as planes, slopes. Some factors of there unknown
planes are estimated together with the calibration parameters.
The parameters of a plane j are described as
S;=\S>
(2)
where S lf S 2 and 5 3 are the direction cosines of the plane's
normal vector and S 4 is the negative orthogonal distance
between the plane and the coordinate system origin. The
observation equation for an point i expressed by its
coordinates x , » T,, z t lying on plane j has the form
SljX i +S 2j y l +S 3 jZ i +S 4 j=0
(3)
Figure 3. Navigator position RMS for X, Y, and Z direction
Note that the direction cosines must satisfy the following unit
length constraint
3. ERROR REVOERY MODEL
3.1 Geo-Referencing of LiDAR Measurements
As already mentioned, it is necessary to compute the laser point
geo-referencing that represent mathematical models. The
geo-referencing of the laser points is viewed as a function of
the observation from the above parameters estimated. The
LiDAR geo-referencing equation in a local reference frame can
be given in eq. 1:
(1)
Xi
m
X
m /
Ax
■°T
y t
=
Y
+c
Ay
+ R m Rs
m
0
3.
Z
Az
Ip])
where:
x r y r z i
X, Y,Z
=the laser footprint position in the mapping
frame
=position of the phase center of GPS antenna
in the mapping frame
(4)
Combining equation (1) with equation (2) consist of the form
that constraint conditions and laser points position as a function
of the systematic errors:
F(0,X) = 0 (5)
where, O is the observations, X is the systematic errors.
The geo-referencing of the laser points in the laser coordination
system is viewed as a function of the GPS, INS, range,
scan-angle, and the systematic biases. In section 2, the
systematic biases are selected from bore-sight angles, ranging
biases, and scanning angle biases. After adding the systematic
errors to the equation (1), the geo-referencing of the laser
points is changed by the following form:
Ax, Ay, Az =ever arm vector from the phase center of
X
m
X
m /
Ax
GPS antenna to laser scanner center
y
=
Y
+RL
Ay
R" mu =the rotate matrix between the IMU frame
z
Z
Az
+ AR m R„ARR,
(6)
and the mapping frame described by roll, pitch
and yaw observation
=a priori known rotation matrix from the IMU
frame to the LS coordinate frame that depends
on the mounting situation.
=laser scanner rotation
cos# -sin#
sin# cos#
y =the LiDAR encoder angular value
p =the LiDAR range at time t
3.2 Recovery Function Model
The following model is based on constraining the target objects
to the surface extracted from the laser points and known
AR„ =
0),(p,K
=the range bias
=rotation matrix with alignment error a
defined in section 2
=bore-sight rotation matrix
=bore-sight angles
Since the equation (6) is non-linear and each laser point
position is represented by more than one observation, the
adjustment model must be used. Substituting the equation (6) to