The International Archives of the Photogrammetry, Remote Sensing and Spatial Information Sciences. Vol. XXXVII. Part B5. Beijing 2008
Measurements in the vicinity and outside the edges of the
whiteboard are likewise omitted. Figure 6 presents the
distributions of all distance residuals of the examined image
sequence, grouped by the integration time they were captured
with. Obviously, they all exhibit a negative offset from zero in
the range of centimetres.
Figure 5. Sample frames from the image sequence used for the
integrated calibration of both the interior orientation and the
ranging system, with detected targets indicated in red.
[pixel!
1: 4x4.2ms
2: 4x4.2ms
3: 4x4.2ms
Xo ± O x o
84.298 ±.041
84.700 ± .028
85.327 ±.047
yo± Ovo
-54.404 ± .033
-54.500 ± .030
-54.357 ±.050
f ± Of
200.459 ± .031
200.743 ± .035
200.884 ± .048
a 3 ± Oa3
-0.382 ±.001
-0.386 ±.001
-0.373 ±.001
4: 4x2.2ms
5: 4x10.2ms
6: 4x20.2ms
Xo ± 0x0
84.695 ± .039
84.653 ± .039
84.860 ±.038
yo ± OyO
-54.521 ±.043
-54.202 ± .037
-54.631 ±.036
f ± Of
200.740 ± .035
200.656 ± .042
200.935 ± .040
a 3 ± Oa3
-0.387 ±.001
-0.389 ±.001
-0.378 ±.001
Table 2. Interior orientation and radial distortion parameter,
adjusted for groups of 1000 frames featuring uniform
integration times that are indicated in the table header.
Due to the limited extents of the used whiteboard, the whole
distance measurement range cannot be covered. Nevertheless,
the confrontation of the residuals with their reference values
reveals parts of the periodic non-linearities reported in literature.
See Figure 7 for details, bearing in mind that mean residuals for
reference values above 2.5m are weakly determined.
Figure 6. Distribution of distance deviations, grouped by
integration time.
Figure 7. Histogram of derived distances and residuals
confronted with them.
Figure 8. Histogram of observed amplitudes and their relation
to range residuals.
The comparison of residuals to the corresponding amplitude
observations discovers a very clear relation, supported by an
almost equal distribution of residuals over the encoding range.
While range measurements with amplitudes above 2><10 4 do not
appear to be sensitive to changes in the signal strength, there is
a very strong effect on values below, see Figure 8.
Examining the influence of the angle of incidence on the
residuals does not provide much information. The seeming
strong relation above 75gon is supported by few residuals only,
see Figure 9.
As a consequence of using only a subset of the range
observations, the utilised residuals are not equally distributed
on the sensor, which may be verified on Figure 10. Still, each
pixel is related to at least 4000 residuals, which gives
significance to their mean: with respect to the distances derived
from the exterior orientation, the range observations are
generally too large, still getting worse towards the principal
point, roughly.
Histogram of Incidence Angles
Figure 9. Histogram of incidence angles and their
confrontation with ranging residuals.
Figure 11 presents the distribution of pixel footprints on the
whiteboard. The precisely circular holes prove the high quality
of target centroiding. As large-scale images have mainly been
captured in the centre, the density of residuals decreases
towards the borders of the test field. For that reason, the
apparent effect of radially increasing mean residuals is rather
little supported. The absence of scattering is proved again, as
there are no circular structures around the voids of the target
areas.