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4. Microtransduction: actuation and sensing                      223






         The tip angle produced through torsion about the longitudinal x-axis is:





         Equation (4.95) has taken into account that for a thin cantilever, the torsional
         rigidity is 4 times higher than the bending one – see Chapter 2. By taking the
         ratio of the two tip angles results in:





         As a consequence,        for               is solution to Eq. (4.96)) and:





         When                  which gives:





         5       PIEZOELECTRIC (PZT) TRANSDUCTION

             The piezoelectric  materials  have  the property of becoming  electrically
         polarized in  the  presence of  an  externally applied  load/deformation. The
         degree of polarization is proportional to the level of mechanical deformation,
         as  well as is dependent  on  the direction  of  the applied strain.  This
         mechanical-to-electrical energy conversion  is  known as direct  piezoelectric
         effect, and  crystals  such  as the quartz  naturally  exhibit  this  property.
         Piezoelectric  materials are  also  capable  to responding in a linear  manner  to
         the reverse  excitation, in  the  sense  that  external application  of a  field  will
         generate mechanical deformation through the reverse piezoelectric effect
         (also called electrostriction). Examples of piezoelectric materials largely
         utilized in  industrial/research  applications are polycrystalline  ceramic
         materials  such as  the  PZT (lead zirconate  titanate) or semi-crystalline
         polymers  such  as the PVDF  (polyvinylidene  fluoride). For  such  materials,
         the  component  dipoles  (molecules that  are partly charged positively and
         partly charged negatively) are randomly arranged in a lattice, but application
         of an external  electric field to such an unpoled structure will pole it,  namely
         arrange and direct the dipoles about a direction parallel to that of the external
         field, as sketched in Fig. 4.40.
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