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  • 标题:Some issues regarding the calibration of the terrestrial laser scanner Leica Scanstation C10.
  • 作者:Antanaviciute, Urte ; Obuchovski, Romuald ; Parseliunas, Eimuntas Kazimieras
  • 期刊名称:Geodesy and Cartography
  • 印刷版ISSN:1392-1541
  • 出版年度:2013
  • 期号:September
  • 语种:English
  • 出版社:Vilnius Gediminas Technical University
  • 摘要:Terrestrial 3D laser scanners (TLS)--a new class of survey instruments--have become popular and are increasingly used in providing as-built and modelling data in various applications, including land surveying, archaeological studies, architecture, bridge structures, and highway surveys. These scanners could measure thousands of data points (distance, angle, and reflected return signal power) per second and generate a very detailed "point cloud" data set. In addition, these measurements are performed much faster than traditional geodetic surveys in most cases; therefore, terrestrial laser scanning has become an additional surveying technique in the geodesy over the last several years. However, in contrast to traditional geodetic instruments (e.g. total stations, levels, Global Navigation Satellite Systems), accuracies and the systematic errors of most of the available laser scanners are not well-known. An investigation and analysis are essential to use terrestrial laser scanners for high precision applications (e.g. engineering surveying). In order to minimise the systematic influence of the instrumental errors, scanners have to be calibrated and observations have to be corrected on the basis of the calibration parameters (Ingensand 2006). The standardised calibration routines exist for the traditional geodetic and photogrammetric instruments. In the context of TLS, the reliable accuracy assessment is rather complicated due to the fact that laser scanners are constructed in a way completely different from the traditional survey equipment. (Pfeifer, Briese 2007). The accuracy specifications given by laser scanner producers in their publications and pamphlets are not comparable. Experience shows that the given accuracy parameters should not be trusted in some instances; besides, accuracy of these instruments --which are built in small series--varies from instrument to instrument and depends on individual calibration. Much work has been done on point-based TLS calibration by exploiting their similarities with theodolites or a total station (Parian, Grun 2005; Lichti, Franke 2005; Lichti, Licht 2006; Lichti 2007; Reshetyuk 2006). Self-calibration approaches have recently been investigated by a number of researchers and can be categorised according to the type of targeting. Two types are reported: signalised point targets and planar features. The common thread between both approaches is the collection of a highly redundant set of spherical observations (range, horizontal direction and elevation angle) from different locations in a strong geometric configuration. (Bae, Lichti 2007; Dorninger et al. 2008; Schneider 2009). The application of mentioned procedures requires a laboratory or a calibration room with known geometrical parameters of targets or planar features. The mentioned calibration procedures use the 3D coordinates of the measured points; however, the laser scanners actually measure the ranges, vertical and horizontal angles (Pfennigbauer, Ullrich 2010). Therefore, it is important to evaluate each measured parameter separately (Chow et al. 2010).
  • 关键词:Geodesy;Optical scanners;Scanning devices

Some issues regarding the calibration of the terrestrial laser scanner Leica Scanstation C10.


Antanaviciute, Urte ; Obuchovski, Romuald ; Parseliunas, Eimuntas Kazimieras 等


Introduction

Terrestrial 3D laser scanners (TLS)--a new class of survey instruments--have become popular and are increasingly used in providing as-built and modelling data in various applications, including land surveying, archaeological studies, architecture, bridge structures, and highway surveys. These scanners could measure thousands of data points (distance, angle, and reflected return signal power) per second and generate a very detailed "point cloud" data set. In addition, these measurements are performed much faster than traditional geodetic surveys in most cases; therefore, terrestrial laser scanning has become an additional surveying technique in the geodesy over the last several years. However, in contrast to traditional geodetic instruments (e.g. total stations, levels, Global Navigation Satellite Systems), accuracies and the systematic errors of most of the available laser scanners are not well-known. An investigation and analysis are essential to use terrestrial laser scanners for high precision applications (e.g. engineering surveying). In order to minimise the systematic influence of the instrumental errors, scanners have to be calibrated and observations have to be corrected on the basis of the calibration parameters (Ingensand 2006). The standardised calibration routines exist for the traditional geodetic and photogrammetric instruments. In the context of TLS, the reliable accuracy assessment is rather complicated due to the fact that laser scanners are constructed in a way completely different from the traditional survey equipment. (Pfeifer, Briese 2007). The accuracy specifications given by laser scanner producers in their publications and pamphlets are not comparable. Experience shows that the given accuracy parameters should not be trusted in some instances; besides, accuracy of these instruments --which are built in small series--varies from instrument to instrument and depends on individual calibration. Much work has been done on point-based TLS calibration by exploiting their similarities with theodolites or a total station (Parian, Grun 2005; Lichti, Franke 2005; Lichti, Licht 2006; Lichti 2007; Reshetyuk 2006). Self-calibration approaches have recently been investigated by a number of researchers and can be categorised according to the type of targeting. Two types are reported: signalised point targets and planar features. The common thread between both approaches is the collection of a highly redundant set of spherical observations (range, horizontal direction and elevation angle) from different locations in a strong geometric configuration. (Bae, Lichti 2007; Dorninger et al. 2008; Schneider 2009). The application of mentioned procedures requires a laboratory or a calibration room with known geometrical parameters of targets or planar features. The mentioned calibration procedures use the 3D coordinates of the measured points; however, the laser scanners actually measure the ranges, vertical and horizontal angles (Pfennigbauer, Ullrich 2010). Therefore, it is important to evaluate each measured parameter separately (Chow et al. 2010).

Some work has been done in distance measurement accuracy evaluation (Salo et al. 2008; Cheok et al. 2007) with the following indication that the accuracy depends on many factors such as scanner model, range measuring method, target properties and etc. Angle measurement accuracy tests indicate that the angle measurement accuracy (especially vertical one) depends on the design of a laser beam deflecting unit (Schneider, Schwalbe 2008; Reshetyuk 2009, 2010).

It is important to point out that no standard measure of the scanner performance and method for its evaluation exists (Lichti 2010). The method proposed by the authors of this paper allows evaluating the distance and angle measurement accuracies under real environmental conditions. Additionally, the proposed method does not require a special calibration laboratory; consequently, a standard geodetic baseline could be used.

1. Calibration of the distance measuring device of the terrestrial laser scanner at the cyclic error determination baseline

The calibration of the distance measuring device of the terrestrial laser scanner Leica Scanstation C10 was performed using the cyclic error determination baseline at the Calibration Laboratory of the Research Institute of Geodesy of Vilnius Gediminas Technical University (Jokela et al. 2002; Buga et al. 2008, 2011). The cyclic error determination baseline consists of 16 points, distances between which are approx. 1 metre. During the calibration procedure, the terrestrial laser scanner was force-centred at the first mount and distance measurements were performed to the force-centred targets (6 inches in diameter) positioned on the other mount (Fig. 1).

[FIGURE 1 OMITTED]

The point cloud of the each scanned target consists of approx. 39000 points. From these point clouds, the coordinates of the centres of targets were determined using Cyclone software by Leica Ltd. As usual, distances between the scanner and targets were calculated using the formula:

S = [square root of ([([X.sub.t] - [X.sub.s]).sup.2] + [([Y.sub.t] - [Y.sub.s]).sup.2])], (1)

where [X.sub.t] and [Y.sub.t]--coordinates of the target centre, [X.sub.s] and [Y.sub.s]--coordinates of the scanner.

Calibration parameters of the distance measuring device of the laser scanner were evaluated by comparing the calculated distances with known standard distances. Further data handling and calculations were performed using the standard methodology of the numerical data processing of the calibration results (Putrimas 2010). The final results are presented in Table 1.

Table 1 indicates that systematic errors are relatively small (less than 1.3 mm) in short distance measurements. These errors are slightly greater for short distance (up to 3 metres) measurements.

Systematic distance measurement errors are shown in Figure 2.

The constant R of the terrestrial laser scanner was calculated using all systematic errors of the measured distances and is equal to -0.4 mm. Figure 2 shows that systematic error changes from -1.3 mm to +0.4 mm.

[FIGURE 2 OMITTED]

2. Calibration of the distance measuring device of the terrestrial laser scanner at Kyviskes Calibration Baseline

Calibration of the distance measuring device of the terrestrial laser scanner Leica Scanstation C10 was also performed at Kyviskes Calibration Baseline. This base consists of 6 pillars erected in a straight line with the distance between the first and the last pillar amounting to 1320 m. Distances between the inner pillars are as follow: 1-2 - 100 m, 2-3 - 260 m, 3-4 - 760 m, 4-5 - 180 m, 5-6 - 20 m (Joke la et al. 2002; Buga et al. 2008, 2011). During the calibration procedure, measurements of five different sectors of the calibration base were performed. The longest chosen distance amounted to 260 metres, i.e. did not exceed the maximal possible range of the terrestrial laser scanner. The measurements were performed between pillars 1-2; 2-3; 4-5; 4-6 and 5-6. Laser scanner and targets were force-centred on the pillars (Fig. 3).

[FIGURE 3 OMITTED]

The calibration results are presented in Table 2.

As Table 2 provides, systematic errors change from -16.9 mm to 3.7 mm and the constant R of the terrestrial laser scanner is equal to -8.5 mm. The standard deviation of systematic errors change from 0.00 mm to 0.5 mm and the standard uncertainty of the mean systematic error value has a range from 0.0 mm to 0.1 mm. A noticeable increase of the systematic error values could be observed in distances above 100 m. Systematic error values are shown in Figure 4.

As the analysis of calculated distance measurement accuracies suggests, the systematic error tends to linearly increase with growing distance. For distances up to 100 metres, this error does not exceed 3.7 mm and, therefore, conforms to the technical specification of the investigated laser scanner, i.e. 4 mm/50 m.

[FIGURE 4 OMITTED]

3. Calibration of the horizontal angle measuring device of the terrestrial laser scanner

Calibration of the horizontal angle measuring device of the terrestrial laser scanner Leica Scanstation C10 was also performed at Kyviskes Calibration Baseline. The experiment was carried out by placing targets on pillars 5 and 6. The accuracy of horizontal angle measurement was estimated from three different scanner positions with different angles with respect to the mentioned targets. Measured distances were corrected for systematic errors as described in the previous chapter. Based on trigonometric formulas, the comparison of measured and known (reference) horizontal angles was performed.

The measured angle between TLS and targets can be estimated by applying the coordinates of the targets and scanner:

[MATHEMATICAL EXPRESSION NOT REPRODUCIBLE IN ASCII] (2)

here [MATHEMATICAL EXPRESSION NOT REPRODUCIBLE IN ASCII]- coordinates of the scanner position, [MATHEMATICAL EXPRESSION NOT REPRODUCIBLE IN ASCII]- coordinates of the targets. The elements of the formulae (2) are shown in Figure 5.

[FIGURE 5 OMITTED]

The well-known cosine formulae were used to calculate value of the angle [beta]:

[S.sub.3.sup.2] = [S.sub.1.sup.2] + [S.sub.2.sup.2] - 2[S.sub.1][S.sub.2] cos([beta]) (3)

and

[[beta].sub.t] arccos [S.sub.1.sup.2] + [S.sub.2.sup.2] - [S.sub.3.sup.2] / 2[S.sub.1][S.sub.2]. (4)

The above formulae (4) should be used two times in carrying out the calibration process. The first time they should be used when the measured angle [[beta].sub.i] is calculated from laser scanner data (coordinates). And the next time the formulae (4) should be used for reference or real angle determination from the known reference distance [S.sub.3] and measured corrected distances [S.sub.1] and [S.sub.2].

Calibration results of the horizontal angle measuring device are presented in Table 3.

As Table 3 provides, systematic errors vary from -3.5" to 0.6" depending on the angle sharpness. The angular constant of the terrestrial laser scanner is equal to A = -1.3". The standard deviation of systematic errors varies from 2.1" to 5.1" and the standard uncertainty of the mean systematic error value has a range from 0.9" to 2.1".

Conclusions

The calibration method of the horizontal angle measuring device is proposed. It is based on placing the scanner in front of the calibration base reference line and measuring the angle in front of this line. The reference value of this angle is obtained from the lines of a triangle applying cosine formulae.

It is estimated that the accuracy of the investigated scanner distance measuring device is noticeably (from ~4 mm to ~14 mm) decreases for the distances more than 100 metres. It is necessary to perform more tests with several scanners in order to determine whether it is a constructive defect or a random scanner deficiency.

The accuracy parameters of the investigated laser scanner Leica Scanstation C10 correspond with the accuracy criteria specified in the scanner technical specification.

Caption: Fig. 1. The cyclic error determination baseline mounts with targets

Caption: Fig. 2. Graphical representation of systematic errors of the terrestrial laser scanner distance measuring device based on the calibration at the cyclic error determination baseline.

==

Caption: Fig. 3. Target scanned at Kyviskes calibration baseline

Caption: Fig. 4. Graphical representation of systematic errors of the terrestrial laser scanner distance measuring device based on the calibration at Kyviskes Calibration Baseline

Caption: Fig. 5. Scheme for determination of the horizontal angle measured by TLS

doi: 10.3846/20296991.2013.840356

References

Bae, K. H.; Lichti, D. D. 2007. On site self-calibration using planar features for terrestrial laser scanners, International Archives of Photogrammetry, Remote Sensing and Spatial Information Sciences, vol. 36 (Part 3/W52): 14-19.

Buga, A.; Jokela, J.; Putrimas, R. 2008. Traceability, stability and use of the Kyviskes calibration baseline--the first 10 years, in Proc. of the 7th International Conference Environmental Engineering, 22-23 May, 2008, Vilnius. Vilnius: Technika, 1274-1280.

Buga, A.; Jokela, J.; Putrimas, R.; Zigmantiene, E. 2011. Analysis of EDM instruments calibration at the Kyviskes calibration baseline, in Proc. of the 8th International Conference Environmental Engineering, 19-20 May, 2011, Vilnius. Vilnius: Technika, 1301-1305.

Cheok, G. S.; Saidi, K. S.; Lytle, A. M. 2007. Evaluating a ranging protocol for 3D imaging systems, in 24th International Symposium on Automation & Robotics in Construction, 19-21 September, 2007, Kochi, Kerala, India, 81-87.

Chow, J.; Lichti, D.; Teskey, B. 2010. Self-calibration of the Trimble (Mensi) GS200 Terrestrial Laser Scanner, in ISPRS Commission V Mid-Term Symposium "Close range Image Measurement Techniques", 22-24 June, 2010, Newcastle upon Tyne, United Kingdom (in Press).

Dorninger, P.; Nothegger, C.; Pfeifer, N.; Molnar, G. 2008. On-the-job detection and correction of systematic cyclic distance measurement of terrestrial laser scanners, Journal of Applied Geodesy 2(4): 191-204. http://dx.doi.org/10.1515/JAG.2008.022

Ingensand, H. 2006. Methodological aspects in terrestrial laser-scanning technology, in Proceedings of the 3rd IAG Symposium of Geodesy for Geotechnical and Structural Engineering and 12th FIG Symposium on Deformation Measurements, 22-24 May, 2006, Baden, Austria, [CD].

Jokela, J.; Buga, A.; Putrimas, R. 2002. Analysis of repeated calibration of Kyviskes baseline, Geodezija ir kartografija [Geodesy and Cartography] 28(4): 37-41.

Lichti, D. D.; Franke, J. 2005. Self-calibration of the iQsun 880 laser scanner, in Optical 3-D measurement techniques VII, vol. 1. Vienna, Austria, 112-121.

Lichti, D. D.; Licht, M. G. 2006. Experience with terrestrial laser scanner modelling and accuracy assessment, The International Archives of the Photogrammetry, Remote Sensing and Spatial Information Sciences, vol. 36 (Part 5): 155-160.

Lichti, D. D. 2007. Error modelling, calibration and analysis of an AM-CW terrestrial laser scanner system, ISPRS Journal of Photogrammetry and Remote Sensing 61(5): 307-324. http://dx.doi.org/10.1016/j.isprsjprs.2006.10.004

Lichti, D. D. 2010. Terrestrial laser scanner self-calibration: correlation sources and their mitigation, ISPRS Journal of Photogrammetry and Remote Sensing 65(1): 93-102. http://dx.doi.org/10.1016/j.isprsjprs.2009.09.002

Parian, A. J.; Grun, A. 2005. Integrated laser scanner and intensity image calibration and accuracy assessment, The International Archives of the Photogrammetry, Remote Sensing and Spatial Information Sciences, vol. 36 (Part 3/ W19): 18-23.

Pfeifer, N.; Briese, C. 2007. Geometrical aspects of airborne laser scanning and terrestrial laser scanning, IAPRS, vol. 36 (Part 3/W52): 311-319.

Pfennigbauer, M.; Ullrich, A. 2010. Improving quality of laser scanning data acquisition through calibrated amplitude and pulse deviation measurement, in SPIE Proceedings, vol. 7684: Laser Radar Technology and Applications XV http://dx.doi.org/10.1117/12.849641.

Putrimas, R. 2010. Elektroniniu tolimaciu kalibravimo metodika ETKM-2010. IV leid. Vilniaus Gedimino technikos universitetas.

Reshetyuk, Y. 2006. Calibration of terrestrial laser scanners Callidus 1,1, Leica HDS 3000 and Leica HDS 2500, Survey Review 38(302): 703-713. http://dx.doi.org/10.1179/003962606780674763

Reshetyuk, Y. 2009. Self-calibration and direct georeferencing in terrestrial laser scanning: Doctoral Thesis in Infrastructure, Royal Institute of Technology (KTH), Stockholm, Sweden [online], [cited June 2013]. Available from Internet: http:// kth,divaortal,org/smash/record,jsf?pid=diva2:139761

Reshetyuk, Y. 2010. A unified approach to self-calibration of terrestrial laser scanners, ISPRS Journal of Photogrammetry and Remote Sensing 65(5): 445-456. http://dx.doi.org/10.1016/j.isprsjprs.2010.05.005

Salo, P.; Jokinen, O.; Kukko, A. 2008. On the calibration of the distance measuring component of a terrestrial laser scanner, in IAPRS (Ed.). Proceedings of the 21th ISPRS Congress, Silk Road for Information from Imagery, Vol. 37-B5, Beijing, China, 1067-1071.

Schneider, D.; Schwalbe, E. 2008. Integrated processing of terrestrial laser scanner data and fisheye-camera image data, The International Archives of the Photogrammetry, Remote Sensing and Spatial Information Sciences, vol. 37 (Part B5): 1037-1043.

Schneider, D. 2009. Calibration of a Riegl LMS-Z420i based on a multi-station adjustment and a geometric model with additional parameters, International Archives of Photogrammetry, Remote Sensing and Spatial Information Sciences, vol. 38 (Part 3/W8): 177-182.

Urte ANTANAVICIUTE. Senior Data Operator. SE "GIS-CENTRAS". Seliu g. 66, LT-08109 Vilnius, Lithuania. Ph +37062065308, e-mail: u.antanaviciute@gis-centras.lt

MSc at VGTU (2013).

Research interests: calibration of geodetic instruments, geodesy, terrestrial laser scanning, cartography.

Romuald OBUCHOVSKI. Doctor of Technological Sciences. Vilnius Gediminas Technical University. Dept of Geodesy and Cadastre, Sauletekio al. 11, LT-10223 Vilnius, Lithuania. Ph +370 5 274 4703, Fax +370 5 274 4705, e-mail: romuald.obuchovski@vgtu.lt

MSc at VGTU (2002).

Research interests: geomagnetic field, gravity field, terrestrial laser scanning.

Eimuntas Kazimieras PARSELIUNAS. Professor, Doctor. Department of Geodesy and Cadastre, Vilnius Gediminas Technical University, Sauletekio al. 11, LT-10223 Vilnius, Lithuania. Ph +370 5 274 4703, Fax +370 5 274 4705, e-mail: eimis@vgtu.lt.

Doctor (1992). Habilitation procedure in 2008. Author of two teaching books and more than 50 scientific papers. Participated in many international conferences.

Research interests: graphs theory in geodesy, adjustment of geodetic networks, geoinformation systems.

M. G. Darius POPOVAS. Assistant Professor. Department of Geodesy and Cadastre, Vilnius Gediminas Technical University, Sauletekio al. 11, LT-10223 Vilnius, Lithuania. Ph +370 5 274 4703, Fax +370 5 274 4705, e-mail: darius.popovas@vgtu.lt.

Doctor of Technological Sciences (VGTU), 2011.

Research interests: terrestrial laser scanning, GNSS.

Dominykas SLIKAS. Doctoral student. Department of Geodesy and Cadastre, Vilnius Gediminas Technical University, Sauletekio al. 11, LT-10223 Vilnius, Lithuania. Ph +370 5 274 4703, Fax +370 5 274 4705, e-mail: dominykas.slikas@vgtu.lt.

MSc at VGTU (2007).

Research interests: calibration of geodetic instruments, engineering geodesy, airborne and terrestrial laser scanning.

Urte Antanaviciute (1), Romuald Obuchovski (2), Eimuntas Kazimieras Parseliunas (3), M. G. Darius Popovas (4), Dominykas Slikas (5)

Vilnius Gediminas Technical University, Sauletekio al. 11, LT-10223 Vilnius, Lithuania E-mails: 1urtean@gmail.com; 2romuald.obuchovski@vgtu.lt; 3eimis@vgtu.lt; 4darius.popovas@vgtu.lt; 5dominykas.slikas@vgtu.lt (corresponding author)

Received 28 August 2013; accepted 18 September 2013
Table 1. Final results pertaining to calibration parameters of the
distance measuring device of the laser scanner based on calibration
at the cyclic error determination baseline

Segment    Standard     Mean measured    Systematic error
number    distance, m    distance, m     of distances, mm

   1        0.9993          1.0005             -1.2
   2        2.0000          2.0011             -1.1
   3        3.0006          3.0019             -1.3
   4        4.0007          4.0014             -0.7
   5        4.9990          4.9986             +0.4
   6        5.9981          5.9987             -0.6
   7        6.9995          7.0004             -0.9
   8        7.9967          7.9970             -0.3
   9        8.9990          8.9993             -0.3
  10        9.9999         10.0002             -0.3
  11        10.9976        10.9981             -0.5
  12        11.9995        11.9999             -0.4
  13        12.9980        12.9980              0.0
  14        13.9992        13.9989             +0.3
  15        15.0038        15.0040             -0.2
                                             R = -0.4

Segment   Standard deviation of    Standard uncertainty
number     systematic error, mm     of mean systematic
                                      error value, mm

   1               0.4                      0.1
   2               0.4                      0.1
   3               0.1                      0.0
   4               0.3                      0.1
   5               0.5                      0.2
   6               0.3                      0.1
   7               0.3                      0.1
   8               0.4                      0.1
   9               0.2                      0.1
  10               0.5                      0.2
  11               0.2                      0.1
  12               0.2                      0.1
  13               0.2                      0.1
  14               0.1                      0.0
  15               0.9                      0.3

Table 2. Final results of calibration parameters pertaining to
the distance measuring device of the laser scanner based on the
calibration at Kyviskes Calibration Baseline

Segment   Reference     Mean measured    Systematic error
number    distance, m    distance, m     of distances, mm

   1        20.0102        20.0095              0.7
   2       100.1632        100.1595             3.7
   3       180.0930        180.1070            -14.0
   4       200.1032        200.1191            -15.9
   5       260.0118        260.0287            -16.9
                                             R = -8.5

Segment   Standard deviation of    Standard uncertainty
number     systematic error, mm     of mean systematic
                                      error value, mm

   1               0.0                      0.0
   2               0.2                      0.1
   3               0.4                      0.1
   4               0.4                      0.1
   5               0.5                      0.1

Table 3. Final results pertaining to calibration parameters of the
horizontal measuring device of the laser scanner based on the
calibration at Kyviskes calibration baseline

Measured     Mean values of      Reference angle        Angle
 angle     the measured angle    [degrees] '"      systematic error
              [degrees]'"                                 "

   1       17     40     3.4    17   40    4.0          0.6
   2       26     8      32.4   26   8    31.4          -1.0
   3       49     19     30.2   49   19   26.7          -3.5
                                                      A = -1.3

Measured    Standard deviation     Standard uncertainty of
 angle     of systematic error   mean systematic error value
                    "                         "

   1               2.6                       1.0
   2               5.1                       2.1
   3               2.1                       0.9
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