Calibration of a Terrestrial Laser Scanner - Institute of Geodesy and ...
Calibration of a Terrestrial Laser Scanner - Institute of Geodesy and ...
Calibration of a Terrestrial Laser Scanner - Institute of Geodesy and ...
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4Static <strong>Laser</strong> ScanningThis chapter discusses the post-processing <strong>of</strong> 3D point clouds as applied to static laser scanning. Staticlaser scanning implies that the objectsto be scanned <strong>and</strong> the laser scanner do not move relative to eachother during the data acquisition process. Post-processing <strong>of</strong> 3D point clouds requires s<strong>of</strong>tware packagesto derive the final products, e.g. 3D models. Since the implemented algorithms in these s<strong>of</strong>tware packagesare not fully automated, the operator has to assist the s<strong>of</strong>tware. Thus, the process <strong>of</strong> deriving the finalproduct based on the 3D point cloud is time-consuming. The time ratio between post-processingscanning point clouds <strong>and</strong> data acquisition can be upaspects <strong>of</strong> data processing, registration, <strong>and</strong> modelingto 10 : 1or more. The following<strong>and</strong> visualization.<strong>of</strong> lasersections cover some4.1 Data Processing<strong>Laser</strong> scanning is one <strong>of</strong> the fastest data acquisition techniques in geodesy <strong>and</strong> generates a hugenumber <strong>of</strong>points, which describe the environment, in a short time. However, data acquisition produces blunders <strong>and</strong>noise within the point clouds. Noise can be distinguished in white noise <strong>and</strong> coloured noise. Here, noise isassumed to be white noise <strong>and</strong> Gaussian noise. The following sections givean overview <strong>of</strong> the conceivableerrors <strong>and</strong> error sources. They result in noisy data <strong>and</strong> have to be processed by applying special filtering<strong>and</strong> noise reduction techniques.4.1.1 Blunder DetectionThe laser scannersystem acquires data within a distance <strong>and</strong> an intensity interval. Sometimes, only datawithin a specific range regarding distance <strong>and</strong> intensity values are required. The pointswhich fulfil theserequirements can easily be separated from the points that do not fulfil the requirements by introducingminimum <strong>and</strong> maximum limits for both range <strong>and</strong> intensity data, a threshold:rangemm