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handbook of modern sensors

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7.5 Optical Sensors 275<br />

Therefore, electric pulses injected into the waveguide’s coaxial conductor produce<br />

mechanical twist pulses which propagate along the waveguide with the speed <strong>of</strong> sound<br />

specific for its material. When the pulse arrives at the excitation head <strong>of</strong> the sensor,<br />

the moment <strong>of</strong> its arrival is precisely measured. One way to detect that pulse is to<br />

use a detector that can convert an ultrasonic twitch into electric output. This can be<br />

accomplished by piezoelectric <strong>sensors</strong> or, as it is shown in Fig. 7.24, by the magnetic<br />

reluctance sensor. The sensor consists <strong>of</strong> two tiny coils positioned near two permanent<br />

magnets. The coils are physically coupled to the waveguide and can jerk whenever<br />

the waveguide experiences the twitch. This sets up short electric pulses across the<br />

coils. The time delay <strong>of</strong> these pulses from the corresponding excitation pulses in the<br />

coaxial conductor is the exact measure <strong>of</strong> the ring magnet position. An appropriate<br />

electronic circuit converts the time delay into a digital code representative <strong>of</strong> a position<br />

<strong>of</strong> the permanent magnet on the waveguide. The advantage <strong>of</strong> this sensor is in its high<br />

linearity (on the order <strong>of</strong> 0.05% <strong>of</strong> full scale), good repeatability (on the order <strong>of</strong><br />

3 µm), and long-term stability. The sensor can withstand aggressive environments,<br />

such as high pressure, high temperature, and strong radiation. Another advantage <strong>of</strong><br />

this sensor is its low-temperature sensitivity which by careful design can be achieved<br />

on the order <strong>of</strong> 20 ppm/ ◦ C.<br />

Applications <strong>of</strong> this sensor include hydraulic cylinders, injection-molding machines<br />

(to measure linear displacement for mold clamp position, injection <strong>of</strong> molding<br />

material, and ejection <strong>of</strong> the molded part), mining (for detection <strong>of</strong> rocks movements<br />

as small as 25 µm), rolling mills, presses, forges, elevators, and other devices where<br />

fine resolution along large dimensions is a requirement.<br />

7.5 Optical Sensors<br />

After mechanical contact and potentionometric <strong>sensors</strong>, optical <strong>sensors</strong> are probably<br />

the most popular for measuring position and displacement. Their main advantages are<br />

simplicity, the absence <strong>of</strong> the loading effect, and relatively long operating distances.<br />

They are insensitive to stray magnetic fields and electrostatic interferences, which<br />

makes them quite suitable for many sensitive applications. An optical position sensor<br />

usually requires at least three essential components: a light source, a photodetector,<br />

and light guidance devices, which may include lenses, mirrors, optical fibers, and so<br />

forth. An example <strong>of</strong> single- and dual-mode fiber-optic proximity <strong>sensors</strong> are shown<br />

in Figs. 4.17 and 4.18 <strong>of</strong> Chapter 4. Similar arrangements are <strong>of</strong>ten implemented<br />

without optical fibers when light is guided toward a target by focusing lenses and is<br />

diverted back to detectors by the reflectors. Currently, this basic technology has been<br />

substantially improved. Some more complex and sophisticated products have evolved.<br />

The improvements are aimed to better selectivity, noise immunity, and reliability <strong>of</strong><br />

the optical <strong>sensors</strong>.<br />

7.5.1 Optical Bridge<br />

The concept <strong>of</strong> a bridge circuit, like a classical Wheatstone bridge, is employed in<br />

many <strong>sensors</strong> and the optical sensor is a good example <strong>of</strong> that. One such use shown in

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