manner as for calibration but on the next day and after sufficient
zoom action. This time, the 3D co-ordinates were "traced back"
to the image co-ordinates using all the calibrated parameter
values. These image co-ordinates were then compared with the
"measured" image co-ordinates to derive root mean squared
errors. These are shown in Table 3. We can say that this r.m.s.e.
is attributed to the error of repeatability, the error of the
calibrated parameters and the error of target image location. If we
take off the latter part from the RMS., the repeatability ranges
from 0.17 to 0.35 pixel (RMS).
Table 3. Repeatability over Zoom (pixels)
5.4
10.8
Focal Settings (mm)
16.2
21.6
43.2
RMS:c
0.37
0.33
0.17
0.18
0.27
RMSy
0.33
0.21
0.17
0.18
0.37
RMSc
0.35
0.28
0.17
0.18
0.33
8.2 Repeatability test using a single target
A simple method had in fact been implemented to assess zoom
repeatability before the above experiment was performed. The
method used a single stable target. The stable camera imaged the
targets many times and before each time the zoom was adjusted
away and back. The repeatability was computed as standard
deviation of the target image position. Results for the tested focal
settings were shown in Table 4. Since only a single target was
used in this method, the results should only be interpreted as
indictive. Nevertheless, the inconsistency between Table 3 and
Table 4 somehow indicates that the repeatabilities at various focal
settings do not repeat themselves very well and that the factors of
repeatability are complex. 9
Table 4. Repeatability over Zoom by Single Target (pixel)
Focal Settings (mm)
5.4
43.2
RMSx
0.11
0.19
RMSy
0.09
0.27
RMSc
0.10
0.21
9 CONCLUSIONS AND FUTURE WORK
The repeatability of the calibrated zoom camera system against
zooming is about 0.4 pixel (gross with assessment error). This
level meets the requirement of the terrestrial image based system
for which the camera system is employed. This level of accuracy
for zoom cameras is believed to be also satisfactory for many
measurement applications. This will enable zoom lens cameras to
gain a better share in photogrammetric application, which is now
much dominated by fixed lens cameras.
The radial lens distortion is very significant, especially for short
focal lengths. It can amount 0.2 pixels at 43 mm focal length to
1.7 pixels at 5.4 mm focal length. This amount is fortunately
compensatable with the three radial lens distortion terms. The
decentering lens distortion is much smaller than the radial type,
but still significant compared with the 0.08 pixel random error
level of the calibration. The magnitude of lens distortion
normally does not pose problems in practice. What really matters
is the calibratability or stability of the distortion.
The camera-on-theodolite calibration method has proved very
effective and efficient for calibrating zoom CCD cameras. In
particular, it has proved to be very suitable for calibrating this
camera-theodolite combined unit. As the combined unit was
calibrated in exactly the same set-up as it will be employed for
measurement application, the 0.4 pixel repeatability figure can be
taken for the prediction of the accuracy level achievable by the
system.
By the time of writing, experiments are still going on to obtain
more data at more focal settings. Modelling the orientation
parameters with focal length will be attempted. Constrained
calibration with fewer free parameters, fewer images and a single
target will be experimented.
Fully automated calibration is not yet realised by the time of
writing, but it remains one of the goals of the project. This is of
importance considering the fact that the zoom mechanics tends to
ware and more frequent calibration is required for a zoom camera
than for a fixed lens camera. Thanks to the camera-on-theodolite
calibration method, which lends itself to automation, the date for
reporting a full automatic calibration should not be long.
ACKNOWLEDGEMENT
The authors would like to thank Measurement Devices Limited
for lending the camera, and colleagues Jim Dudley, Ms Daoxiang
Gong, and Darryl Newport for assistance during the experiments.
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