Page 345 - Microsensors, MEMS and Smart Devices - Gardner Varadhan and Awadelkarim
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ACOUSTIC  WAVE PROPAGATION     325

                                                2
  where  e kij  is  the  piezoelectric  constant  in  units of C/m ,  E k  is  the  kth  component  of  the
                  E
  electric  field,  and c ijkl is  measured  either  under  a zero  or a constant  electric  field.
    In  nonpiezoelectric  materials,  the  electrical  displacement  D  is  related  to  the  electric
  field  applied  by
                                  D=s re 0E                           (10.13)

  where  e r  is the relative  permittivity,  formerly  called the dielectric  constant,  and e 0  is the
  permittivity  of  vacuum, now known as  the  electric constant.  For  piezoelectric  materials,
  the  electrical  displacement  is extended  to:

                                           S
                               Di  = e iklS kl+e ikE k                (10.14)
         S
  where e ik is  measured  at constant  or  zero  strain.
    Equations  (10.12)  and  (10.14)  are  often  referred  to  as  piezoelectric  constitutive
  equations.  In  matrix  notation,  Equations  (10.12)  and  (10.14)  can  be  written  as  (Auld
  1973b):

                                             T
                              [T] =  [c][S]–[e ]E
                               D  =  [e][S ] +        [e]E            (10.15)
  where,  [e]  is  a  3 x  6  matrix  with  its elements  depending  on the  symmetry  of the  piezo-
                    T
  electric  crystal  and  [e ]  is  the  transpose  of  the  matrix  [e].  For  quartz  having  a trigonal
  crystal  classification, the  [e]  matrices  are

                         /  e {[  -e n  0  e\4  0     0  \
                    [e] =   0     0   0    0       -e 14     -e 11    (10.16)
                         V  0     0 0 0         0     0
  The  difference  between  poled  and  naturally  piezoelectric  materials  is  that  in  the  former,
  the  presence  of  a large  number  of  grain boundaries  and its  anisotropic  nature would  lead
  to  a  loss  of  acoustic  signal  fidelity  at  high  frequencies.  This  is  one  of  the  reasons  SAW
  devices  are,  usually,  only fabricated  out  of  single-crystal  piezoelectrics.


  10.5  ACOUSTIC     WAVE PROPAGATION

  10.5.1  Uniform  Plane  Waves  in a Piezoelectric  Solid:
         Quasi-Static  Approximation


  For  the  numerical  calculations  of  acoustic  wave  propagation,  the  starting  point  is  the
  equation  of  motion  in  a piezoelectric  material  (Auld  1973a)

                            pu i  =  T ij.j  i,  j  =  1,2, 3         (10.17)

  where,  p  is  the  mass density,  and  u i  is  the  particle  displacement.
                                                        2
    In  tensor  notation,  the  two  dots  over  a  symbol  denotes  a /at 2  and  a  subscript  i
  preceded  by  a comma  denotes  a/ax i.  The  piezoelectric  constitutive equations  in  (10.15)
  are rewritten  in  tensor notation:
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