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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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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.

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