International Archives of the Photc
Figure 12. Barrage structure measured from the panoramic
stereo model in Figure 11.
3. RESULTS AND DISCUSSION
In order to verify the procedure, we compared geometries of
some structures, which were measured both with tacheometer
and from photogrammetric documents. The structures were one
barrage system (B1) and two terrace Systems (T1 and T2). The
measurement geometry is presented in Figure 13. The barrage
system and its measured points are shown in Figure 12.
As a kind of rule of thumb one can expect precisions of stereo
photogrammetric measurements using following formula:
a = 2 . 3X
c : (1)
zZ
dY = . dy
e ,and (2)
E m
ua =".
eB 3)
in which X and Y are the coordinates parallel to the image
plane, Z is the coordinate in viewing direction (i.e. the
distance), C is camera constant, B is the effective base of
photography.
We consider here roughly that the precision dx or dy of any
measured image coordinate is one pixel and the precision of the
parallax measurement dpx is 1.4 pixels. The measurement
geometry in our experiment is presented in Table 1 and Figure
13. and the expected precisions in Table 2. In case of our
experiment, the camera constant C is 1400 pixels, the base B is
7.5 m and the distances to measured structures varied between
45 — 100 m.
The results indicate that panoramic images can be applied for
archaeological survey. With regard to measured locations of
structures, the external accuracy meets the expectations:
Barrage Bl in Tables 2 and 3, and all structures in Figure 13.
The measured bias in case of barrage Bl, i.e. the mean of
coordinate differences between both measurements are within
the range of expected precisions.
With regard to measured points, the internal precision meets the
expectations as well: Barrage Bl in Tables 2 and 4, and in
Figure 14. Both measured shapes of Barrage BI appear similar,
whereas in case of Terrace T1, the shapes become scattered
when measured from images. However, the repeatability 1s
good. This indicates that the interpretation on images becomes
»grammetry, Remote Sensing and Spatial Information Sciences, Vol XXXV, Part
BS. Istanbul 2004
vague or uncertain compared to the interpretation in sifu with
tacheometer.
Table 1. The measurement geometry.
c B dx dy dpx
[pixel] [m] [pixel] [pixel] [pixel]
1400 7.5 ] 1 1.4
Table 2. Expected precisions in the experiment.
Z dX dY dZ
[m] [m] [m] [m]
Barrage Bl 45 0.03 0.03 0.27
Terrace T1 60 0.04 0.04 0.49
Terrace T2 100 0.07 0.07 1.35
1 / ss
sat Jj >
vef. ol
p- À
if
Figure 13. Measurement geometry of presented
photogrammetric survey of terrace and barrage structures. For
comparison, the structures are measured with tacheometer. The
base of the stereo photography is 7.5 m and the distance here to
the furthest structure is 100 m.
Table 3. The bias in Barrage Bl.
N (-X) Z (-Y) E (-Z)
[m] [m] [m]
Bias -0.01 0.11 -0.17
When imaging distances increase, the uncertainties in measured
distances increase. According to the Formula 3 the effect is
squared with respect to the distance (Z). This effect becomes
clear in case of Terrace T2 (Fig. 15) where the shapes become
highly scattered when measured from images.
However, with respect to repeated image measurements 1 and 2,
the range of scattering is higher than the expected 1.7 m in
Table 2. This increased scattering can be explained by higher
uncertainty in finding exactly corresponding points on stereo
images when the structure is lineated parallel to the image base.
Instead of point wise measuring, the structures should be
interpreted on images as linear features, which would lead to
less scattered shapes.
In case a DEM is available, these linear features can be
measured on single images and the 3-D determination would
proceed by intersection with the DEM surface. This alternative
method is called mono plotting (Viite). However, mono plotting
is inaccurate, since it assumes that the structures lie flat on
terrain.
The proper way would be to measure the structures as
corresponding linear features on at least two images and then
determine the corresponding 3-D structure by intersection in
space.