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Where am I? Sensors and Methods for Mobile Robot Positioning

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112 Part I <strong>Sensors</strong> <strong>for</strong> <strong>Mobile</strong> <strong>Robot</strong> <strong>Positioning</strong><br />

4.2 Phase-Shift Measurement<br />

The phase-shift measurement (or phase-detection) ranging technique involves continuous wave<br />

transmission as opposed to the short pulsed outputs used in TOF systems. A be<strong>am</strong> of <strong>am</strong>plitudemodulated<br />

laser, RF, or acoustical energy is directed towards the target. A small portion of this wave<br />

(potentially up to six orders of magnitude less in <strong>am</strong>plitude) is reflected by the object's surface back<br />

to the detector along a direct path [Chen et al., 1993]. The returned energy is compared to a<br />

simultaneously generated reference that has been split off from the original signal, <strong>and</strong> the relative<br />

phase shift between the two is measured as illustrated in Figure 4.21 to ascertain the round-trip<br />

distance the wave has traveled. For high-frequency RF- or laser-based systems, detection is usually<br />

preceded by heterodyning the reference <strong>and</strong> received signals with an intermediate frequency (while<br />

preserving the relative phase shift) to allow the phase detector to operate at a more convenient lower<br />

frequency [Vuylsteke, 1990].<br />

n=8<br />

n=7<br />

n=6<br />

n=5<br />

Tx<br />

x<br />

n=1 n=2<br />

n=3 n=4<br />

Liquid<br />

Surface<br />

Rx<br />

d<br />

Figure 4.21: Relationship between outgoing <strong>and</strong> reflected wave<strong>for</strong>ms, where x is the<br />

distance corresponding to the differential phase. (Adapted from [Woodbury et al.,<br />

1993].)<br />

The relative phase shift expressed as a function of distance to the reflecting target surface is<br />

[Woodbury et al., 1993]:<br />

1 4%d<br />

<br />

where<br />

1 = phase shift<br />

d = distance to target<br />

= modulation wavelength.<br />

(4.1)

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