CIP A 2003 XIX th International Symposium, 30 September - 04 October, 2003, Antalya, Turkey
The scans were made with a MENSI S-25 laser scanner which
is based on the triangulation technique from two different
locations, parallel to the rock face.
Triangulation measurement system works by geometric relation
with angle of laser beam, recorded position of laser spot on the
CCD and distance of CCD base (Figure 2).
Figure 2. Triangulation methods for range acquisition (Beraldin
et. al., 2000)
Triangulation system performs more accurate and fast
measurement at moderate range (0.8-10m) and a CCD camera
of scanner must detect structured light. Thus the measurement
distance was set about 5m and the experiment was conducted
under the cloudy sky.
This measurement system consists of computer hardware and
software which are for backup the large point data, and laser
scanner. The type of data being returned by a laser scanner is a
dense point cloud which means 3D position of object. The file
(format is *.pts) in X, Y and Z coordinates which are relative to
the scanner’s position are taked by Rapidform2002 which is
software to visualize and to generate DSM with the point data
(Figure 3). To avoid the shadow, scanning is conducted from
two positions and the two stereo images were obtained. It must
be conformed a complete image.
. * * S *. lì 4. * <
. - -Jir-i *s* f ” -> OS. S
pmi» ~"E ■ » «,
Figure 3. Screen capture from Rapidform2002 program for
building digital surface model using the data
acquired from laser scanner
2.2 Digital Photogrammetry
For estimating the accuracy of digital stereo photogrammetry,
the stereo image was obtained for the same area where laser
scanning was conducted. To decrease the radial distortion
which becomes larger and larger where located far from the
center of lense, we took stereo images in the position where
triangular shape was made at the center of image.
Canon EOS D30 was used with 22.7 x 15.1 mm CCD. The
resolution of image was 2,160 x 1,440 pixel and focal length
was about 5.6 m.
15 targets were attached around the triangular shape of image
for the control points and the check points and the 3D
coordinate of the points was measured by 5” theodolites DT5S).
Initial position to take the images and targets are shown at
Figure 4. The origin was positioned behind the rock face to
prevent Z-coordinate being negative number.
To obtain interior and exterior orientation which establishes
the position and orientation of the bundle of rays with respect to
the object space coordinate system, bundle adjustment was
applied (Mikhail et. al., 2001). Table 1 shows the results.
Left Camera
(0,1490,8000)
Left Theodolite
* ^(0,1415,8000)
Jf
Right Camera
(2077.1690.8000)
Right Theodolite
(2077.1612.8000)
Figure 4. Three dimensional coordinate system : distributed
solid circles represent targets (units are mm)
Camera
Parameters
Left
Right
•
0.227811 rad
0.201134 rad
•
-0.139705 rad
0.205790 rad
•
0.040883 rad
-0.052426 rad
X«
-21.581 mm
2068.103 mm
Y 0
1497.158 mm
1704.751 mm
Z 0
8045.914 mm
8019.272 mm
x 0
5.956283 pixel
0.154158 pixel
yo
-2.359040 pixel
-0.895909 pixel
Zo
27.908419 mm
28.15702227 mm
Table 1. Interior and exterior orientation parameters of
reference surface determined by EOS D30
camera(units are radian and mm, respectively)