Page 118 - Instrumentation Reference Book 3E
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Sensor practice 103

              The  constant  a  depends  on  many  factors   PZT  material  itself  contributes  only  of  the
             including the geometry of the crystal, position  of   order of 0.03 of critical damping. If no additional
             electrodes, and material used.  Typical materials   damping is added, PZT transducers must not be
             now  used  (natural quartz  is  less  sensitive and,   used  too  close  to  their  resonant  frequency.
             therefore, less applicable) include barium titanate   Mounting arrangements within the case will also
             with  controlled  impurities,  lead  zirconate,  lead   add  some  additional  damping.  Some  designs
             niobate,  and  many  that  are  trade  secrets.  The   make use of an additional spring element; some
             material  is made  from loose  powder  that, after   use an additional spring to precompress the PZT
             shaping, is fired at very high temperature. Whilst   element so that it remains biased in compression
             cooling, the  blocks  are  subjected  to  an  electric   under  all  working  amplitudes:  this  makes  for
             field that polarizes the substance.      more linear operation.
              The sensitivity of these so-called “PZT mater-   Typical  sensor  sensitivities  range  from  0.003
             iais” is temperature-dependent through the charge   pC/m s-~ up to 1000pC/m s-~, implying that the
             sensitivity  and  the  capacitance  value,  both  of   following pre-amplifier units will also need to vary
             which alter with temperature. These changes do   considerably.
             not follow simple linear laws. Such materials have
             a critical temperature,  called the “Curie point.”   6.3.4.4  Amplifiers for piezoelectric sensol’s
             They  must  never  be  taken  above  it.  The Curie
             point varies from  120°C for the simpler barium   An amplifier for reading out the state of the PZT
             titanate  Corms  ranging  up  to  values  close  to   sensor is one that has very high input impedance,
             600°C. For  the  interested  reader  more  explan-   an adequate frequency response, and low output
             ation  is  to be  found  in  Bruel  and Kjaer  (1976):   impedance.  Adjustment  of  gain  and  filtering
             Endevco (1980), Harris and Crede (1961), Klaasen   action and integration to yield  velocity and dis-
             (1978):  and  Trampe-Broch  (1980),  and  in  the   placement are usually also needed to provide easy
             detailed  information  provided  by  the  makers  of   use for a variety of applications. Figure 6.19 is a
             PZT materials.                           typical  system incorporating  most  features  that
               To read the charge of a PZT sensor an electro-   might be needed.
             nic amplifier that  converts charge magnitude  to   The amplifier could be designed to see the sen-
             a  voltage  equivalent  is  used.  The nature  of  the   sor  either  as  a  voltage  source  or  as  a  charge
             system provides no true DC response.     source. The latter is preferred for, using modern
               In  practice  the  PZT  sensors used  to  measure   electronic-feedback  operational  amplifier  tech-
             acceleration  can  be  operated  down  to  around   niques, the effect of cable, sensor, and amplifier
             0.1 Hz, dependent  on the  amplitude to be meas-   capacitances  can  be  made  negligible (which, in
             ured. With natural resonant frequency that can be   the  voltage-reading  method,  is  not  the  case).
             made relatively very high (up to 100,000 Hz in some   Cable  length  is,  therefore,  of  no  consequence.
             designs), PZT sensors provide a useful frequency   This is justified as follows.
             range  that  can  cover  most  vibration  needs.  The   Figure 6.20 is the relevant equivalent circuit for
             system response, however, relies  not only on the   a  PZT  accelerometer  that  is  connected  to  an
             sensor but upon  the cables and the pre-amplifier   operational  amplifier  (the  pre-amplifier)  via  a
             used with the PZT unit.                  cable. It includes the dominant capacitances that
               The PZT material can be used in pure compres-   occur.
             sion; shear,  or  bending,  to  produce  the  charge.   It can be shown (see Trampe-Broch (1980) for
             Figure 6.12 gives some examples of commercially   example) that the use of feedback in this way and
             available PZT accelerometers. The sensor design   a very high amplifier gain A gives
             is  amenable  to  the  combination  of  three  units
             giving  the  three  translation  components  of
             vibration.













             Figure 6.19  Blockdiagram of vibration measuring system showing functions that may be required. Courtesy, Bruel & Kjaer.
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