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The platinum resistance thermometer

This type of thermometer, devised by Callendar in 1877, uses the change in the resistance of a platinum wire with temperature to measure the change in temperature. The equation for such a change is:

Rθ = Ro(1 + αθ + βθ2)

where <θ is the temperature change and α and β are constants, β being much smaller than α. We therefore ignore the term β2 and assume that the resistance of the wire varies uniformly with temperature: a is the temperature coefficient of resistance of the material.
For platinum a = 3.8x10-4 oC-1.

A simple form of the platinum resistance thermometer is shown in Figure 1. It consists of a platinum wire wound non- inductively on a mica former and held in a glass tube by silica spacers. The resistance of the wire is measured with a Wheatstone bridge network and to allow for the change in resistance of the leads a set of dummy leads are included in the opposite arm of the bridge (see Figure 2).


This type of thermometer has a large range, from -200 oC to +1100 oC and this can be extended by the use of different wires. Bronze has a range starting at -260 oC and using carbon temperatures as low as –270 oC can be measured.

The advantages of the resistance thermometer are its convenient size, wide range and high sensitivity (±0.000 05 oC). It can only be used for steady readings, however, and is not direct-reading.

The accuracy obviously depends on how accurately the bridge can be balanced.

 
 
 
© Keith Gibbs 2013