Page 124 - Introduction to Autonomous Mobile Robots
P. 124

Perception


                                                                 D                             109
                           Transmitter
                                                                                      P
                                    L                                                 Target

                                         Phase                            Transmitted Beam
                                       Measurement                        Reflected Beam

                           Figure 4.9
                           Schematic of laser rangefinding by phase-shift measurement.


                           Amplitude [V]

                                                            Phase [m]

                                      0   θ

                                                λ                            Transmitted Beam
                                                                             Reflected Beam
                           Figure 4.10
                           Range estimation by measuring the phase shift between transmitted and received signals.



                           Phase-shift measurement. Near-infrared light (from a light-emitting diode [LED] or
                           laser) is collimated and transmitted from the transmitter in figure 4.9 and hits a point P in
                           the environment. For surfaces having a roughness greater than the wavelength of the inci-
                           dent light, diffuse reflection will occur, meaning that the light is reflected almost isotropi-
                           cally. The wavelength of the infrared light emitted is 824 nm and so most surfaces, with the
                           exception of only highly polished reflecting objects, will be diffuse reflectors. The compo-
                           nent of the infrared light which falls within the receiving aperture of the sensor will return
                           almost parallel to the transmitted beam for distant objects.
                             The sensor transmits 100% amplitude modulated light at a known frequency and mea-
                           sures the phase shift between the transmitted and reflected signals. Figure 4.10 shows how
                           this technique can be used to measure range. The wavelength of the modulating signal
                                               ⋅
                                                       c
                           obeys the equation c =  f λ   where   is the speed of light and f the modulating frequency.
                                                            λ
                           For   = 5 MHz (as in the AT&T sensor),   = 60 m. The total distance D'  covered by the
                              f
                           emitted light is
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