Page 394 - Microsensors, MEMS and Smart Devices - Gardner Varadhan and Awadelkarim
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374    IDT MICROSENSORS

   The  two  reflectors are  located  such that the  time delay at  room  temperature  TQ is

                           T\  =  1 us  and  T 2 =  1.1 us             (13.37)

   Then,
                                   TO =  0.1  us                       (13.38)

                                                                 th
   The transmitted FM signal is pulse-modulated with a time duration of  1760  of a  second.
   The carrier  frequency  varies  linearly  from  905  MHz to 925 MHz during the  period.  The
   parameters  in Equation (13.22)  for  the  FM  signal  are

                                 =  905 MHz                            (13.39)
                                            3
                            fi/2n  =  1.2 x  10~  MHz/us               (13.40)
   In  operation,  the  distance  between  the  two  antennas is  1 to  2  meters  so  that  r e  can  be
   neglected  compared  with  x\  or  12- The  temperature  variation can  be  in  the  range  0  to
   200 °C. The  first  and  second  terms in Equation (13.30)  can  now be  calculated



                                       6
                        = 2n x 905 x 10  -  1.2 x  10 -3  x  1.05/2    (13.41)
                                      6
                       =  2n  x 905 x 10

  So,  the  approximation  in  Equation (13.30)  is  clearly justified.  From  Equations  (13.34),
  (13.36),  and (13.38),  the constant a  is

                           a  =  3.06  angular degrees/°C              (13.42)

  The  resolution  of  the  phase  shift  is  1° so that the  resolution of  the  temperature reading is
  given  by  Equation (13.35)  as
                                     =  0.33°C                        (13.43)

  The experimental  calibration  is done in a temperature-controlled  chamber called  a Delta
  9023, (Figure  13.14).
     A digital hand-held thermometer (Keruco Instruments Co.) with an accuracy of ±0.2 °C
  is  taken  as  the  temperature  standard.  The  temperature  range  in  the  experiment  is  from
  room  temperature  (near  20 °C)  to  a  maximum  of  140 °C.  The  straight  line  theory,  as
  shown  in  Figure  13.15,  fits  well  the  experimental  points  of  phase  against  temperature.
  The  equation  for  the  line  in  Figure  13.15  is  obtained  by  the  least  mean  square method
  and  is given by
                                ?> =  2.897-49.1                      (13.44)

  The value of the slope coefficient  a (2.89) is in good agreement with that (3.06) estimated
  from  Equation (13.42). The  root  mean square (rms) error of the phase difference  is equal
  to 0.78°,  which corresponds  to  an rms error  of 0.26 °C.
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