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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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3.2 Distance Measurement System 41The first one has to be proven by making periodic distance calibrations, called scale factor, <strong>and</strong> are causedbythe oscillator. Thesecond one can have different reasons that are caused by the environment such astemperature changes inside <strong>and</strong>/or outside the laser scanner.Variations in frequency results in variations in the distance measurements. However, it is not possible todistinguish between variations in distances <strong>and</strong> variations in the frequency because several parametersinterfere with each other <strong>and</strong> lead to distance variations, e.g.conditions, properties <strong>of</strong> the target (such as colour, material, roughness), angleadditive constant, scale factor, atmospheric<strong>of</strong> incidence.Thus, thedetermination <strong>of</strong> frequency variations has to be done directly by using an electronic unit for frequencymeasurements, cf. Section 3.1.4.The important frequency for the resolution <strong>of</strong> the distance measurement system is the modulated frequency<strong>of</strong> the fine channel component, i.e. high frequency signal 'hfs'. Thus, the investigationis focused on thismodulation frequency. In the experimental setup, the laser beam is aligned towards the diode, the signal <strong>of</strong>the frequency is detected <strong>and</strong> the real frequency is derived, cf. Figure 3.6. The investigation was performedwithin an observation period <strong>of</strong> nearly three hours with a samplinginterval <strong>of</strong> one minute. One assumesa time-dependent <strong>and</strong> temperature-dependent behaviour. Thus, the temperatureinside the laser scanneris recorded additionally. The temperature <strong>of</strong> the environment is constant because the investigation wascarried out in an air-conditioned laboratory.transmitter temperaturedifference to nominal frequency (« 45 MHz)Figure 3.20:Development <strong>of</strong> the frequency <strong>of</strong> high frequency signal 'hfs' <strong>and</strong> the internal temperature <strong>of</strong> the laserscanner.Figure 3.20 shows the time variations in both the modulation frequency 'hfs' <strong>and</strong> the internal temperature<strong>of</strong> the laser scanner, i.e. transmitter temperature. First, the deviations <strong>of</strong> the 'hfs' to the reference frequencycan be seen. Second, the 'hfs' reaches a constant frequency after nearly two hours in operation <strong>and</strong> showsa deviation to the nominal frequency <strong>of</strong> nearly 50 Hz. Third, the behaviour <strong>of</strong> the internal temperature <strong>of</strong>the laser scanner correlates to the frequency behaviour: an increasing temperature leads to a decreasingdeviation between real <strong>and</strong> nominal frequency, that means the real frequency is also increasing becausethe difference to the nominal frequency is calculated by subtracting the real frequencyfrom the nominalfrequency, <strong>and</strong> vice versa. The nominal frequency is defined by /hfs=44.781250 MHz.Based on the given nominal frequency /hfs <strong>and</strong> the real frequency / a scale factor rrif for the correction <strong>of</strong>a distance measurement caused by the difference <strong>of</strong> the real frequency to the nominal frequencycan bederived with [Joeckel <strong>and</strong> Stober, 1991]-/hfs /rrif 1 = '(3.6)/Applying this formula to all acquired real frequencies <strong>of</strong> the modulation frequency'hfs' one can achieve amaximum scale factor <strong>of</strong> 3.2 ppm. The constant frequency after two hours shows a value <strong>of</strong> —1.2 ppm. Con¬sidering the working range <strong>of</strong> the laser scanner <strong>of</strong> 50 m, the differences <strong>of</strong> the modulation frequency result

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