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handbook of modern sensors

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10.3 Mercury Pressure Sensor 341<br />

1 meter at a temperature <strong>of</strong> +4 ◦ C and normal gravitational acceleration. A pascal can<br />

be converted into other units by the use <strong>of</strong> the following relationships (see also Table<br />

A.4 in the Appendix):<br />

1Pa= 1.45 × 10 −4 lb/in 2 = 9.869 × 10 −6 atm = 7.5 × 10 −4 cm Hg.<br />

For practical estimation, it is useful to remember that 0.1 mm H 2 O is roughly equal<br />

to 1 Pa. In industry, another unit <strong>of</strong> pressure is <strong>of</strong>ten used. It is defined as pressure<br />

exerted by a 1-mm column <strong>of</strong> mercury at 0 ◦ C at normal atmospheric pressure and<br />

normal gravity. This unit is named after Torricelli and is called the torr. The ideal<br />

pressure <strong>of</strong> the Earth’s atmosphere is 760 torr and is called the physical atmosphere:<br />

1 atm = 760 torr = 101,325 Pa.<br />

The U.S. Customary System <strong>of</strong> units defines pressure as a pound per square inch<br />

(lb/sq in.) or psi. Conversion into SI systems is the following:<br />

1 psi = 6.89 × 10 3 Pa = 0.0703 atm.<br />

A pressure sensor operating principle is based on the conversion <strong>of</strong> a result <strong>of</strong> the<br />

pressure exertion on a sensitive element into an electrical signal. Virtually in all<br />

cases, pressure results in the displacement or deformation <strong>of</strong> an element, having a<br />

defined surface area. Thus, a pressure measurement may be reduced to a measurement<br />

<strong>of</strong> a displacement or force, which results from a displacement. Thus, we recommend<br />

that the reader also becomes familiar with displacement <strong>sensors</strong> covered in Chapter<br />

7 and force <strong>sensors</strong> <strong>of</strong> Chapter 9.<br />

10.3 Mercury Pressure Sensor<br />

A simple yet efficient sensor is based on the communicating vessels principle (Fig.<br />

10.1). Its prime use is for the measurement <strong>of</strong> gas pressure. A U-shaped wire is<br />

immersed into mercury, which shorts its resistance in proportion with the height<br />

<strong>of</strong> mercury in each column. The resistors are connected into a Wheatstone bridge<br />

circuit, which remains in balance as long as the differential pressure in the tube is<br />

zero. Pressure is applied to one <strong>of</strong> the arms <strong>of</strong> the tube and disbalances the bridge,<br />

which results in the output signal. The higher the pressure in the left tube, the higher<br />

the resistance <strong>of</strong> the corresponding arm is and the lower the resistance <strong>of</strong> the opposite<br />

arm is. The output voltage is proportional to a difference in resistances R <strong>of</strong> the<br />

wire arms which are not shunted by mercury:<br />

V out = V R = Vβp. (10.4)<br />

R<br />

The sensor can be directly calibrated in units <strong>of</strong> torr. Although simple, this sensor<br />

suffers from several drawbacks, such as necessity <strong>of</strong> precision leveling, susceptibility<br />

to shocks and vibration, large size, and contamination <strong>of</strong> gas by mercury vapors. 1<br />

1 Note that this sensor can be used as an inclination sensor when pressures at both sides <strong>of</strong><br />

the tube are equal.

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