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Calibration of a Terrestrial Laser Scanner - Institute of Geodesy and ...

Calibration of a Terrestrial Laser Scanner - Institute of Geodesy and ...

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90 5. Kinematic <strong>Laser</strong> ScanningThe accuracy <strong>of</strong> the orientation depends on the accuracy <strong>of</strong> the determination <strong>of</strong> the azimuthal direction tothe sphere <strong>and</strong> the precision <strong>of</strong> the horizontal encoder system.If the scanning pr<strong>of</strong>ilesare not normal tothe moving direction, the misalignment can be corrected mathematically by using control pointspr<strong>of</strong>iles are shifted by a constant angle.This lever arm effect was discussed earlier.since theazimuthal direction(scanning pr<strong>of</strong>iles )A1S |azimuthal direction / ^^^HI(sphere centre) /oicalibration track linemoving directioninital director(azimuth),test trolley(laser scanner)Figure 5.2: Azimuthal orientation <strong>of</strong> the laser scanner. The azimuthal direction to the sphereazimuthal direction for the pr<strong>of</strong>iles can be determined by adding a specific angle (here: 90 °).can be derived <strong>and</strong> the5.1.2 Absolute Position <strong>and</strong> OrientationThe absolute position <strong>and</strong> orientation <strong>of</strong> an object is defined by three coordinates <strong>and</strong> three attitude angles.To measure the six degrees <strong>of</strong> freedom, different sensors <strong>and</strong> instruments can be used, e.g.acceleratorsensors, inclination sensors, tracking total station, global positioning system.Inertial navigation systems(INS) directly provide the desired six parameters.The sensors <strong>and</strong> instruments that should be used <strong>and</strong> areappropriate for the specific application depend on the desired accuracy <strong>and</strong> the environment. If the objectis in motion, these six parameters are time-dependent <strong>and</strong> define the 3D-trajectory.The kinematic application performed on the calibration track line allows for some simplifications.Thetest trolley moving along the track line is forced to run on a fixed track. The trolleydirections. The trajectory <strong>of</strong> the calibration track line is well-known <strong>and</strong> alreadyThis trajectory can be described by variations in the straightness <strong>of</strong> the alignment, bycannot run in otherdiscussed in Section 3.1.1.variations in thevertical alignment <strong>and</strong> by variations in the cant. The verification <strong>of</strong> the deviations <strong>of</strong> the different linearitiesshows only small variations. The measurement <strong>of</strong> the three attitude angles (to, ,trajectory is well-defined. For simplifications, it is also possible to approximate the trajectoryk) is not necessary since theas a constantline, which runs horizontally. The error budget <strong>of</strong> this approximation is in the same order <strong>of</strong> magnitude asthe accuracy <strong>of</strong> the point cloud acquired bythe laser scanner.The absolute position <strong>of</strong> the test trolley moving along the track line is measured bytion. The laser scanner is equipped with a prism holder to attach a prism, which is tracked byan automated total sta¬the total sta¬tion. Since in kinematic applications the synchronization between the distance <strong>and</strong> the angle measurementsystem <strong>of</strong> tracking total stations is <strong>of</strong> importance [Stempfhuber, 2004], asetup for the kinematic applicationis chosen so that the error resulting from a conceivable erroneous synchronization is minimized. The totalstation is positioned in extension from the track line (pillar number 2000, cf. Figure 3.4). The test trolleymovesaway or towards the total station, resulting mostly in varying distances rather than varying angledirections. The setup can be seen in Figure 5.1.

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