30 3. <strong>Calibration</strong> <strong>of</strong> <strong>Terrestrial</strong> <strong>Laser</strong> <strong>Scanner</strong>between the sphere or the prism, one centimeter deviation in distance does not affect the desired parameterssignificantly, <strong>and</strong> the theodolite, calibration parameters can be derived by usingangle measurements <strong>and</strong> simple geometrical relations.the vertical <strong>and</strong> horizontalEach sphere has different calibration parameters. The closeness <strong>of</strong> the calibration parameters <strong>of</strong> all thespheres allowed for the derivation <strong>of</strong> two sets <strong>of</strong> mean values for the diameter <strong>and</strong> the vertical <strong>of</strong>fset (forthe two different sizes). All results showed that the symmetry <strong>of</strong> the diameter <strong>and</strong> the central position <strong>of</strong> theattached adapter are sufficiently adequate. Thus, the spheres, cf. Figure 3.7, can be used for the calibration<strong>of</strong> the laser scanner.Figure 3.7: Sphere used as target for laser scanning. The diameter <strong>of</strong> the shown sphere is approximatelysphere is attached to a prism holder.12 cm. TheThe center point <strong>of</strong> a sphere can be calculated easily. Normally, a minimum number <strong>of</strong> four points satisfythe definition <strong>of</strong> a sphere <strong>and</strong> with laser scanning, many more points than necessary for defining a sphereare generated. The resulting redundancy allows for the derivation <strong>of</strong> the center point via an adjustment.Therefore, the diameter <strong>of</strong> the spheres can be introduced either as an unknown parameteror as a knownconstant. Within the adjustment procedure, blunders are detected automatically. Blunders are presentnormal distances from each point to the sphere surface exceed a user-defined limit, e.g. 5 mm. This parame¬ter is the same as using normalized residuals <strong>and</strong> is introduced because it can be interpreted geometrically.if theMore information concerning the adjustment procedure can be found in Appendix C.The adjustment isiterated until either all points lie within a maximum distance to the surface <strong>of</strong> the sphere, e.g. 5 mm, or untilthe unknowns, i.e. coordinates <strong>of</strong> the center points <strong>and</strong> the diameter, change below a limit, e.g.The diameters <strong>of</strong> the two spheres (12 cm <strong>and</strong> 15 cm) were chosen with respect to practical aspects0.1 mm.<strong>and</strong> withrespect to the minimum angle increments <strong>and</strong> to the beam divergence <strong>of</strong> the laser scanner, respectively. Onone h<strong>and</strong>, the spheres should be small <strong>and</strong> lightweight enough to be moved <strong>and</strong> transported during fieldwork.On the other h<strong>and</strong>, the spheres have to be large enough to be scanned from distances adapted tothe range interval <strong>of</strong> the laser scanner.Thus, the aforementioned diameters for the sphereswere chosen.Additionally, the best possible value for the optimal diameter <strong>of</strong> the spheres can be derived mathematically.[Reshetyuk et al., 2005] found that the optimal diameter for the laser scanners, HDS 3000 <strong>of</strong> HDS LeicaGeosystems <strong>and</strong> Imager 5003 <strong>of</strong> Zoller+Frohlich, has a value <strong>of</strong> 14 cm.
3.2 Distance Measurement System 313.2 Distance Measurement SystemThe distance measurement system <strong>of</strong> the laser scanner Imager 5003 <strong>of</strong> Zoller+Frohlich is based on the prop¬agation <strong>of</strong> the modulated laser light. If the laser beam hits an object in the environment, then the laser beamis partially reflected <strong>and</strong> can be detected by an APD. This photodiode is coupled with a signal amplifier<strong>and</strong> provides a dynamic range in reflectivity from 5% up to 99% [Fröhlich et al., 2000]. The method usedfor determining distances is the phase difference principle, cf. Section 2.1.4. Because <strong>of</strong> the ambiguity insignals, e.g. sine signals, a maximum range by means <strong>of</strong> a modulated wavelength Amax has to be defined.The challenge by defining Amax is to achieve both a long range interval <strong>and</strong> a high resolution in the distancemeasurement. Therefore, a resolution <strong>of</strong> up to 1/8000 <strong>of</strong> Amax is possible, cf. [Rueger, 1996] <strong>and</strong> [Kahmen,1997]. To guarantee long range as well as high resolution, the emitted laser signal is simultaneouslyintensity-modulated with two different sinusoidal frequencies [Fröhlich et al., 2000]. These two frequenciesdefine a coarse channel component, i.e. low frequency signal Tfs', <strong>and</strong> a fine channel component, i.e. highfrequency signal 'hfs'. The detected laser light contains the phase shifts <strong>of</strong> both modulation frequencies:Tfs' limits the maximum range <strong>and</strong> provides a coarse value for the desired distance <strong>and</strong> 'hfs' delivers aprecise but ambiguous range. Depending on the desired maximum range for 'hfs', two different modescan be chosen: mode 'close' (Aifs « 54 m), <strong>and</strong> mode 'far' (Aifs « 108 m). Thus, the distance between thescanner <strong>and</strong> the object is limited to 27 m <strong>and</strong> 54 m, respectively, 'hfs' has a wavelength <strong>of</strong> Ahfs« 6.7m <strong>and</strong>allows for a resolution <strong>of</strong> less than 1 mm. The carrier wave <strong>of</strong> the emitted laser light is in the near infrared(A « 700 nm). Based on constant emitter signals, the intensity <strong>of</strong> the detected light is equivalentto thereflectivity value <strong>of</strong> the object. The simultaneous detection <strong>of</strong> both range <strong>and</strong> reflectance values guaranteesthat they correspond directly to the same data point in 3D. Furthermore, it has to be mentioned that thisdistance measurement system is (mostly) independent <strong>of</strong> the lighting condition, e.g. ambient light, because<strong>of</strong> the active illumination <strong>of</strong> the laser light.The reflectivity <strong>of</strong> an object is not the only parameter which influences the intensity <strong>of</strong> the reflected lasersignal. Other parameters also affect the reflectivity value (/), such as [Gerthsen <strong>and</strong> Vogel, 1993]:• distance d, which is inversely proportional to the square <strong>of</strong> the distance: / ~ 1/d2•angle <strong>of</strong> incidence• surface properties, e.g. colour, roughness, reflectanceThe laser scanner canoperate in two different modes: a so called 'scanningmode' <strong>and</strong> a so called 'staticmode'. The 'scanning mode' means that the deflection unit is rotating. In contrast, the deflectingthe 'static mode' is not rotating <strong>and</strong> the laser beam can be aligned manually. The usual operationunit inmode forthe laser scanner is the 'scanning mode'. Therefore, the laser beam is deflected by the rotating deflectionunit <strong>and</strong> is scanning the 3D environment. The 'static mode' should only be used for investigation <strong>and</strong>calibration purposes <strong>and</strong> for some specific applications because the laser beam is permanently aligned inone direction <strong>and</strong> is reflected by the same object point in the environment. In 'static mode', the laser beamis dangerous for the human eyes since the laser class is 3R <strong>and</strong> can cause permanent damage to the retina,cf. Section 2.1.2.The operator as well as people involved in the surrounding have to wear safety gogglesaccording to laser safety instructions to avoid irreparable accidents concerning human vision. However,some important aspectscan be gained in 'static mode', for example:• precision <strong>and</strong> accuracy•long-run behaviour• frequency stability, e.g. caused bythermal drifts