4.3 Thermal Transducers
4.3.1 Thermal Sensors
i) Thermo-mechanical
sensors
Thermo-mechanical sensing (and actuation) utilize the fact that all materials have a
coefficient of thermal expansion. Consequently, if two different materials are sandwiched
together and undergo a temperature change, movement in the sandwich assembly would
occur. This is the basis for the common bimetallic (or thermal bimorph) sensing and
actuation.
ii) Thermoresistive sensors
Thermoresistive sensors rely on the fact that the resistivity,
ρ
, of most materials changes with
temperature and is shown by the equation
)
1
(
2
bT
aT
R
=
+
=
ρ
where R is the resistivity of the
material at a reference temperature, T (ºC), and a and b are constants specific to the material
being used. The rate of change of resistance with temperature is known as the temperature
coefficient of resistance. Most common materials exhibit an increase in resistance with
temperature (e.g. platinum is particularly linear with temperature). Certain materials – for
example, carbon, some ceramics and most semiconductors used in thermoresistors or
‘thermistors’ – exhibit a decrease in resistance with increasing temperature. They are not as
linear as platinum, but often cheaper to fabricate and easier to integrate with circuitry in
MEMS devices.
iii) Thermocouples
The thermocouple is probably the most common temperature transducer. It consists of a
junction between two different materials and measures the temperature-dependent voltage that
arises across the junction. Semiconductor materials often exhibit a better thermoelectric
effect than metals. Thermocouples have been used in a wide variety of MEMS sensors in an
array arrangement referred to as a thermopile.
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