Page 125 - Introduction to Autonomous Mobile Robots
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                           a)                          b)                                 Chapter 4
                                         Reflected light
                            Rotating  Transmitted light                       c)
                             Mirror
                                         Reflected light

                                    LED/Laser



                               Detector


                           Figure 4.11
                           (a) Schematic drawing of laser range sensor with rotating mirror; (b) Scanning range sensor from EPS
                           Technologies Inc.; (c) Industrial 180 degree laser range sensor from Sick Inc., Germany




                                                 θ
                                D' =  L +  2D =  L +  ------λ                                 (4.9)
                                                 2π

                                      L
                           where D   and   are the distances defined in figure 4.9. The required distance D  , between
                           the beam splitter and the target, is therefore given by
                                     λ
                                D =  ------θ                                                 (4.10)
                                    4π

                           where  θ   is the electronically measured phase difference between the transmitted and
                                                 λ
                           reflected light beams, and   the known modulating wavelength. It can be seen that the
                           transmission of a single frequency modulated wave can theoretically result in ambiguous
                                                         λ
                           range estimates since, for example, if   = 60 m, a target at a range of 5 m would give an
                           indistinguishable phase measurement from a target at 65 m, since each phase angle would
                                                                                 λ
                           be 360 degrees apart. We therefore define an “ambiguity interval” of  , but in practice we
                                                                    λ
                           note that the range of the sensor is much lower than   due to the attenuation of the signal
                           in air.
                             It can be shown that the confidence in the range (phase estimate) is inversely propor-
                           tional to the square of the received signal amplitude, directly affecting the sensor’s accu-
                           racy. Hence dark, distant objects will not produce as good range estimates as close, bright
                           objects.
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