Page 252 - Microsensors, MEMS and Smart Devices - Gardner Varadhan and Awadelkarim
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232    MICROSENSORS

   Platinum  is the  most  commonly  used  metal  in  resistive  temperature  sensors  because  it is
   very  stable  when cycled  over  a very wide operating  temperature  range  of approximately
   —260 to +1700°C, with a typical reproducibility of better than ±0.1  °C. In fact, platinum
   resistors  are defined under a British Standard BS1904  (1964), made to a nominal resistance
   of  100 £2 at  room  temperature,  and  referred  to  as  Pt-100  sensors.  Platinum temperature
                                                         4
   sensors  are very nearly linear, and «T takes a value of  -1-3.9 x  10~ /K and  fa  takes a value
                                                -7
                                                   2
   that  is  four  orders  of  magnitude  lower  at  —5.9 x  10 /K .  In  contrast,  thermistors,  that
   is, resistors formed  from  semiconducting  materials,  such  as sulfides, selenides, or  oxides
   of  Ni, Mn, or Cu, and Si have highly  nonlinear temperature-dependence.  Thermistors are
   generally  described  by the following  equation:
                                                                         (8.3)


   where  the  reference  temperature  is  generally  25 °C  rather  than  0°C  and  the  material
                                                2
   coefficient  ß  is  related  to  the  linear  TCR  by  —B/T .  The  high  negative  TCR  means
   that  the  resistance  of  a  pellet  falls  from  a  few  megaohms  to  a  few  ohms  over  a  short
   temperature range,  for  example,  100°C  or  so.


   8.2.2  Microthermocouples


   Unlike the metal and semiconducting  resistors, a thermocouple  is a potentiometric  temper-
   ature sensor in that an open circuit voltage V T appears when two different  metals are joined
   together  with the junction  held  at a temperature being  sensed  T s  and  the  other  ends  held
   at a reference temperature  T ref  (see  Figure  8.5).
     The  basic principle is known as the Seebeck effect  in which the  metals have a  different
   thermoelectric  power or  Seebeck  coefficient  P;  the thermocouple is conveniently a linear
   device,  with the  voltage  output  (at zero current) being given by

                V T = (V B -  V A) =              = (P B -               (8.4)

   Thermocouples  are  also  widely  used  to  measure  temperature,  and  their  properties  are
   defined  in  British  and  US  standards  for  different  compositions  of  metals  and  alloys,  for


                            Reference junction
                                            MetalB
                                 -o-


                                                        Sensing
                                         Metal A       junction

                                O



   Figure 8.5  Basic  configuration of  a  thermocouple  temperature  sensor  (a  type  of  potentiometric
   thermal  sensor)
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