Page 410 - Microsensors, MEMS and Smart Devices - Gardner Varadhan and Awadelkarim
P. 410

390    IDT  MICROSENSORS

                 0.6

                 0.4

             ^ 0.2
              i
              1
              i»  0
              'i
              5
              >  –0.2

                –0.4

                -0.6
                              0.05       0.1        0.15       0.2
                                      Time (us)

                    1.5

                    1.0-

                 c  5.0-

                 £  0.0
                 Q.
                 23             0.05                 0.15       02
                 1-5.0
                   -1.0-

                   -1.5
                                      Time (us)

  Figure  13.25  Computed  velocity  of  a  particle  at  the  middle  of  the  resonator  at  the  resonant
  frequency.  The  negative  sign  indicates the  up and down  movement  of  the particle  at  the  antinode
  with  reference  to the  substrate plane


                                    V = -                              (13.88)

                                     I  =  v(f)                       (13.89)

  where 0  is related  to the turns ratio of an equivalent acoustic-to-electric  transformer that
  can be written in terms  of  its electromechanical  coupling coefficient  k,  frequency  f 0,  and
  the  total  capacitance  C  of  the  IDT  as

                                          2
                               0 =   j2f 0Ck Apv                      (13.90)
  Hence,  the  mechanical  characteristic  impedance  Z m  =  F/v  of  the  substrate  can  be ex-
  pressed  as an equivalent transmission  line characteristic  impedance  Z 0.  For a substrate of
  density p and effective  cross-sectional  area A, the mechanical impedance for a propagating
   405   406   407   408   409   410   411   412   413   414   415