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handbook of modern sensors

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16.1 Thermoresistive Sensors 463<br />

Table 16.2. Temperature Differences Between IPTS-68 and ITS-90<br />

t 90 ( ◦ C) −10 0 10 20 30 40<br />

T 90 − t 68 ( ◦ C) 0.002 0.000 −0.002 −0.005 −0.007 −0.010<br />

Source: Saunders, P. The International Temperature Scale <strong>of</strong> 1990, ITS-90. WOCE<br />

Newsletter 10, 1990.<br />

some materials. This scale designated Kelvin temperatures by the symbol T 68 and the<br />

Celsius scale by t 68 . The International Committee for Weights and Measures adopted a<br />

new International Temperature Scale (ITS-90) during its meetings in September 1989.<br />

Its Celsius temperature designation is t 90 .The difference between the two scales may<br />

be significant for some precision measurements (Table 16.2).<br />

Equation (3.58) <strong>of</strong> Chapter 3 gives a best fit second-order approximation for<br />

platinum. In industry, it is customary to use separate approximations for the cold<br />

and hot temperatures. Callendar–van Dusen approximations represent the platinum<br />

transfer functions:<br />

For the range from −200 ◦ Cto0 ◦ C,<br />

R t = R 0 [1 + At + Bt 2 + Ct 3 (t − 100)]. (16.10)<br />

For the range from 0 ◦ Cto630 ◦ C, it becomes identical to Eq. (3.58) <strong>of</strong> Chapter 3:<br />

R t = R 0 (1 + At + Bt 2 ). (16.11)<br />

The constants A, B, and C are determined by the properties <strong>of</strong> platinum used in the<br />

construction <strong>of</strong> the sensor. Alternatively, the Callendar–van Dusen approximation can<br />

be written as<br />

[ ( )( ) ( ) t t<br />

t 3 ( )<br />

R t = R 0<br />

{1 ]} t<br />

+ α t − δ<br />

100 100 − 1 − β<br />

100 100 − 1 , (16.12)<br />

where t is the temperature in ◦ C and the coefficients are related to A, B, and C as<br />

(<br />

A = α 1 + δ )<br />

, B=−αδ × 10 −4 , C=−αβ × 10 −8 . (16.13)<br />

100<br />

The value <strong>of</strong> δ is obtained by calibration at a high temperature, [e.g., at the freezing<br />

point <strong>of</strong> zinc (419.58 ◦ C)] and β is obtained by calibration at a negative temperature.<br />

To conform with ITS-90, the Callendar–van Dusen approximation must be corrected.<br />

The correction is rather complex and the user should refer for details to ITS-90.<br />

In different countries, some national specifications are applicable to RTDs. For instance,<br />

in Europe, these are the following: BS 1904: 1984; DIN 43760–1980; IEC 751:<br />

1983. In Japan, it is JIS C1604-1981. In the United States, different companies have<br />

developed their own standards for α values. For example, SAMA Standard RC21-<br />

4-1966 specifies α = 0.003923 ◦ C −1 , whereas in Europe, the DIN standard specifies<br />

α = 0.003850 ◦ C −1 and the British Aircraft industry standard is α = 0.003900 ◦ C −1 .

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