Investigation of error sources measuring deformations of engineering structures by geodetic methods/Inzineriniu statiniu deformaciju matavimu geodeziniais metodais klaidu saltiniu tyrimas/ Inzenierbuvju deformaciju geodezisko merijumu kludu celonu analize/Veaallikate uurimine ehituskonstruktsioonide deformatsioonide mootmisel geodeetilistel meetoditel.
Aksamitauskas, Vladislovas Ceslovas ; Rekus, Donatas ; Cirba, Stasys 等
1. Introduction
Many highway bridges were designed and built years ago for smaller
vehicular loads, those incorporated in the existing odes and standards.
Therefore, the behavior of structural members of these bridges should be
inspected and controlled more carefully (Kudzys 2009).
Construction work starts and finishes with geodetic measurements,
therefore geodetic measurements and labeling are the most important
components of mounting and installation work in construction.
The digital levels represent a breakthrough in leveling techniques
using the innovative concept of reading a bar coded staff. Optical
readings are no longer needed. Experience shows (Fig. 1) that with
digital levels there is up to 50% time saving when compared with
conventional levels. The main reasons are the faster data capture as
well as the shorter time and safer means of data processing, due to the
possibility of saving measured data on storage devices. Digital levels
measure and save the height and the distance to the staff at the press
of a button, and calculate the height of the point. Advantages are that
no readings are required, no copying or writing down and no calculation
by hand (Ingensand 1999).
Digital automatic levels are precise instruments used for precise
leveling. Operation of digital levels is based on the digital processing
of video information from the coded staff. At the beginning of
measurement a visual pointing of the instrument to the surface of
leveling staff is performed. After that the instrument automatically
points the focus of its optical system on the staff surface and then a
rough correlation calculation is performed followed by the precise
correlation. According to the data received in the processor of the
instrument an exact distance from the axes of the instrument to the
surface of the level staff is calculated. According to the information
received by decoding the data from the photoelectric matrix the height
of the placed level is calculated by the processor. During this
operation the coded view of the staff is compared with that saved in the
memory of the instrument. The true staff height position is determined
according to the shift of the image in the photoelectric sensor (pixels)
matrix.
[FIGURE 1 OMITTED]
Precision investigations of a particular model of levels and coded
staffs and digital leveling are necessary. The investigations of
technical, geometrical and methodological parameters of instruments are
also needed. The scope of this work includes application of digital
automatic levels and impact of their accuracy on construction
measurements (Aksamitauskas et al. 2007; 2010).
2. Accuracy investigation of bar code staffs
A set of digital levels includes bar code staffs that have a
significant impact on the digital leveling results. The choice of the
type of staff depends on its length, material and meteorological
factors. One side of a staff has bar code graduations for the digital
leveling, while the other side has the traditional scale (in cm).
The reference bar code of the staff is stored in the device memory
and during the measurement is correlated (compared) with the code view
of the staff in the linear converter (detector). A two-step correlation
is used: exact and approximate. The approximate correlation reduces the
search area and the calculation volume, as well as shortens the
measurement time. The precision correlation determines the exact
position of the code line image with regard to the reference bar code,
i.e. the staff bar code image is equated with the reference bar code.
For this purpose, a linear detector consisting of 256 photodiodes
(pixels) is used. The accuracy depends on the pixel dimensions, their
number and the sensitivity function of the detector. This, in turn,
affects the accuracy of readings obtained in the level indicator
(Krikstaponis 2000; 2001; Becker et al. 1994; Becker 1999).
Usually, during the accuracy control, the effort is made to place
the control staff into a position where it is used during the operation,
i.e. in a vertical position. However, there are cases when the staff is
tested in a horizontal position and such a composition easies
considerably the measurement and reduces the required height of a room.
Possible structural variations of the staff comparators are listed
in Table 1.
Staff calibration is carried out according to the following
principle: the staff in the comparator is moved using a special lifting
system and a step gear. The staff position is read by a laser
interferometer and edges of the staff scale are recorded with a special
charge coupled device (CCD) camera. Automatic climate control system
records the ambient temperature, pressure, humidity, seeing as the staff
length and the laser wave propagation should be reduced taking into
account environmental factors. This whole system is controlled by a
computer program (Giniotis et al. 2007).
The position accuracy of the leveling staff lines is performed by
comparing photogrammetric images of the support and control staffs or
replacing the base measure with photogrammetric support staff image
recorded with a digital camera and transferred to the computer memory.
In this case, the scale line position of the bar code support staff is
compared with the position of the calibrated staff lines using the
analysis window comprising in the recording unit, which includes the
compared lines of both staffs. The scale line positions of both staffs
is evaluated by performing a local (in the area of the compared lines)
correlation analysis of the digital information, and the calibration
result is determined by the difference in readings between the line
positions of the reference and calibrated staffs at the information
extremes of the digital line positions (line edges).
The principle of this device is that for the staff calibration by a
reference measure, a reference (support) staff and a CCD camera are used
relocating them into a number of positions parallel to the staff axes
and recording the line images of both staffs and their positions in
regard to each other. The calibration results are then evaluated
according to the measurements made with an additional scale situated on
the computer screen, determining the digital difference between the
positions of the measured and reference scale lines.
Photoshooting both the reference staff and the staff under
calibration, an additional millimeter scale (or analog staff) is
installed next to the staffs for control. The additional scale is used
to process results of the digital images in the computer. It also allows
for performing readings along the scales between the line positions of
the reference millimeter scale, the reference staff and the staff under
calibration. The scale graduations are read by an indicator connected to
the analyzing window--diaphragm. Instead of the scale, a coordination
grid of the AutoCad software was used in this study. Calibration system
is shown in Fig. 2.
[FIGURE 2 OMITTED]
In the initial position, moving the analyzing window 3 with an
index, the initial position of the staff lines is read. This is done by
setting the window 3 on the initial lines and recording a certain
correlation coefficient value in the computer correlation unit. Then,
using a selected step, the window 3 is moved along the staff image and
the diaphragm position is corrected by moving it along the measuring
staff 1 to the position where the correlation coefficient becomes equal
to the initially selected correlation coefficient. The diaphragm
position is recorded using the scale 2 and index or the computer
graphical coordinate system. Then the same procedure is performed with
the reference view 2, adjusting the diaphragm position in the coordinate
system to the selected correlation coefficient value, only this time
capturing it from the view 2. The difference between the obtained values
shows the linear error of the line positions of the two staffs. The
procedure is repeated to the entire length of the staffs being
calibrated (Aksamitauskas, Rekus 2009).
3. Scale accuracy studies of bar code leveling staffs
A digital camera used to obtain digital images of bar code staffs
should be calibrated and internal orientation elements, the symmetrical
and unsymmetrical distortions, should be determined. The calibration is
carried out by a computer program using a special stand-point with known
point coordinates. The accuracy of the obtained results is then
estimated. The camera calibration results are used for the further image
processing (Suziedelyte-Visockiene 2007).
All photos used in the study were transformed into a plane in order
to eliminate distortion of the camera lens and to make objects in the
photographs more detailed. To assess the calibration accuracy of the bar
code staffs and to obtain the code scale accuracy of the bar code
leveling staffs, experiments were performed transforming parts of the
photos of the digital bar code leveling staffs into digital information
using a specially designed computer program. Fig. 3 shows one of the
code scales used in the study. The highlighted area in the central part
of the code scale indicates the data that was converted into digital
information (the digital matrix). The central part was selected in order
to minimise as much as possible the inaccuracies in the data matrix
(Giniotis et al. 2008b).
[FIGURE 3 OMITTED]
It was experimented by measuring the digital photo fragments of
scales of the bar code leveling staffs in formats: JPEG, BMP 16-bit, BMP
256-bit, BMP 24-bit, BMP MONOCHROME, TIFF and GIFF. The most suitable
format for the determination and investigation of the code scale edges
was 24-bit BMP, as the clearest view of the code scale edge limits
between black and white lines and the lowest distortion in the digital
photos could be obtained (Aksamitauskas, Rekus 2009).
Fig. 4 demonstrates a fragment of the digital matrix, which was
obtained using the specially designed computer program. Darker color
pixels are expressed with smaller numbers, while brighter pixels are
represented by larger numbers. As a result, a boundary between the black
and white line edges or mechanical damages of the code scale can be
identified.
[FIGURE 4 OMITTED]
Using the obtained digital matrix results, it is possible to
identify the line thickness of each scale that is needed for the further
calibration. The line thickness of the code scale was obtained using
AutoCAD software by loading code scale digital matrix results into the
working window. To assess the accuracy of the performed tests, the line
thickness of the code scales were measured with a microscope UIM-21, No.
640072 (Fig. 5).
[FIGURE 5 OMITTED]
The obtained measurement results and their differences are given in
Table 2 and Fig. 6.
The obtained differences No. 1 and No. 2 of the scale No. 1, as
well as difference No. 3 of the scale No. 3 were very large (the
microscope analyses had large errors), therefore they were excluded from
the further analysis. Analysing the other final results, it can be seen
that the min difference is about 2 [micro]m and the max difference does
not exceed 10 [micro]m.
The measurement accuracy in both cases is nearly equal and the
measurement results differ insignificantly. The line thickness of the
code scales determined using a microscope and with AutoCAD software had
an accuracy of few micrometers.
4. Statistical hypothesis testing
The superposition of the measuring line image can be made using the
principle of the highest correlation coefficient by statistically
comparing the digital information received from calibrated and standard
staffs. The statistical assessment of the line position in such case is
performed by stepwise moving the digital information sequence of the
measuring staff in respect to the reference staff and searching for the
best match of the correlation coefficients (Cekanavicius, Murauskas
2004; 2006; Sakalauskas 2003).
The calculation of the correlation coefficients of the digital
information is carried out according to the Eq (1):
r = [S.sub.xy]/[square root of [S.sup.2.sub.x][S.sup.2.sub.y], (1)
where r - correlation coefficient; [S.sup.2.sub.x]--the empirical
variance of the corresponding line; [S.sup.2.sub.y]--the empirical
variance of another line.
A more reliable estimate of the line edges can be determined using
the linear regression approach. The digital information of the line edge
is analysed statistically determining the consistency of these figures
with the rectilinear dependence. During the regression estimations, the
following hypothesis is tested:
[H.sub.0]: [a.sub.x] = [a.sub.y], (2)
while the corresponding averages are not equal with the alternative
hypothesis:
[H.sub.a]: [a.sub.x][not equal to][a.sub.y] (3)
Since the corresponding variances are unknown, the significance
criterion is applied:
T = [bar.x] - [bar.y]/ [square root of
[s.sup.2.sub.x]-[s.sup.2.sub.y]/2] (4)
which is distributed according to the Student's distribution
with v = 2n-2 degrees of freedom, where [H.sub.0] is true; n - the
number of measurements.
Choosing the significance level [alpha], the critical value of
[t.sub.[alpha], 2n-2] is found in the Student's distribution
tables. Then, the hypothesis that the averages are equal is true
(statistical data (measurement results) do not contradict the fact that
the averages are equal).
If [absolute value of T][greater than or equal to] [t.sub.[alpha],
2n-2] the hypothesis that the averages are equal is rejected and the
alternative hypothesis is accepted, i.e., the averages are not equal.
When the significance level [alpha] = 0.05 (the probability that the
conclusions are wrong) [T.sub.0.05, 2x20-2] = 2.024. In the Eq (4),
[bar.x] is the empirical average of the corresponding line, [bar.y] is
the empirical average of another line, [s.sup.2.sub.x] is the empirical
variance of the corresponding line, and [s.sup.2.sub.y] is the empirical
variance of another line (Giniotis et al. 2008a; Skeivalas, Giniotis
2000).
After the mathematical statistical calculations are done, using a
series of data of the coded scale number matrix and obtained variance
and correlation coefficient values, we can accurately identify the line
boundaries of the coded scales between the black and white line edges
and identify mechanical damages of the coded scale.
Using the analysing window and changing its position in the entire
digital information matrix, we can choose and calculate the max
correlation coefficient between the line position coordinate of the
analysed staffs and define the step by which this coordinate differs
from the line coordinate of the reference scale. This step will be equal
to the absolute error of the line position of the calibrated staff.
Calculating these absolute errors for the entire staff length, a
systematic error of the calibrated staff can be determined.
5. Conclusions
The designed computer program allows expressing the digital image
pixel values of the leveling staff code scales with numeric values.
Darker-colored pixels are expressed in terms of smaller numbers, while
brighter pixels are represented by larger numbers.
Using the developed software it is possible to perform accuracy
tests of the line edges of the code scales.
To assess the accuracy of the performed tests, the line thickness
of the code scales were measured with a microscope UIM-21. The min
difference between the two types of measurements was about 2 [micro]m
and the highest difference did not exceed 10 [micro]m.
When all the mathematical statistical calculations are done, using
a series of data of the coded scale number matrix and obtained variance
and correlation coefficient values, an accurate identification the line
boundaries of the coded scales between the black and white line edges
and mechanical damages of the coded scale can be identified.
Initial studies have shown that the digital image analysis is
highly dependent on the light during the photography, the light
reflectance coefficient on the staff surface as well as the surface
cleanliness, the distance between the camera and the staff surface, and
the contrast of the code lines.
doi: 10.3846/bjrbe.2010.26
Received 18 December 2009; accepted 7 October 2010
References
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Table 1. Principal structure of comparators
Placement Used reference Mobile part
Vertical Laser interferometer Calibrated staff
Horizontal Laser interferometer Carriage with CCD camera
and reflecting prism
Vertical, Digital view of the Without a move or with a
horizontal reference staff partial move (when a
digital camera is reset
with a certain step)
Table 2. The line thickness of the bar code scale measured with a
microscope and the AutoCAD environment
Sequence No. Bar code scale Bar code scale Difference
line thickness, line thickness, [DELTA], mm
measured with measured with
UIM, mm AutoCad, mm
Scale No. 1
1 2.0849 1.8497 0.2352
2 1.9216 1.5999 0.3217
3 4.7599 4.7500 0.0099
4 0.9333 1.6000 -0.6667
5 1.8056 1.7997 0.0059
6 1.6090 1.6003 0.0087
7 14.8039 14.8001 0.0038
Scale No. 2
1 1.0481 1.0498 -0.0017
2 0.9557 0.9498 0.0059
3 2.7551 2.7503 0.0048
4 0.9467 0.9502 -0.0034
5 1.0512 1.0495 0.0017
6 0.9905 1.0002 -0.0097
7 8.5549 8.5499 0.0050
Scale No. 3
1 0.6032 0.6003 -0.0029
2 0.4064 0.4009 0.0055
3 1.3362 1.3990 -0.0628
4 0.4578 0.4490 0.0088
5 0.5528 0.5502 0.0026
6 0.4560 0.4505 0.0055
7 4.3949 4.3988 -0.0039
Fig. 6. The errors measured with UIM and AutoCad software in scales
1 (blue column), 2 (yellow column) and 3 (red column)
1 2 3
1 0.2352 -0.0017 -0.0029
2 0.3217 0.0059 0.0055
3 0.0099 0.0048 -0.0628
4 -0.6667 -0.0034 0.0088
5 0.0059 0.0017 0.0026
6 0.0087 -0.0097 0.0055
Note: Table made from bar graph.
Vladislovas Ceslovas Aksamitauskas (1), Donatas Rekus (2), Stasys
Cirba (3)
(1,2) Dept of Geodesy and Cadastre, Vilnius Gediminas Technical
University, Sauletekio al. 11, 10223 Vilnius, Lithuania
(3) Dept of Mathematical Modelling, Vilnius Gediminas Technical
University, Sauletekio al. 11, 10223 Vilnius, Lithuania
E-mails: (1) Ceslovas.Aksamitauskas@vgtu.lt;1 gkk@vgtu.lt;
3mmk@vgtu.lt