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4. Microtransduction: actuation and sensing                      209
         capacitance change when the  relative  angle between the  fixed  and  the  free
         digits varies, according to the equation:




         The gaps  form an  equivalent  capacitor  whose  change in  capacitance is  the
         sum of  the individual  capacitance  changes, so  that the  total  capacitance
         variation is:







         The total  capacitance  change can  be  transformed in  voltage by  proper
         inclusion  of  the capacitors in  an external electric  circuit.  The voltage
         variation is expressed as:





         3.4     Out-of-the-Plane Microcantilever-based Transduction

             The electrostatic  attraction can  also be  utilized in transduction
          applications that are based on out-of-plane relative motion, such as the case
          is with  microcantilevers. Figure  4.30  illustrates this principle  whereby a
          microcantilever will bend towards an underlying pad of length  either when
          the two  parts are  charged  externally  with  equal and  opposite  charges, or
          when bending of the microcantilever is  achieved externally, and  the change
          in gap between the  two  conjugate  parts is  monitored by  a variation  in
          capacitance. In  essence, the  problem  here is  one  resembling the  transverse
          principle of  transduction, but  the  major difference,  which  is  also
          computationally paramount, consists in the gap not being constant along the
          overlapping region. Moreover, determining the  basic  relationship  between
          the capacitance  change  and the gap change,  which is fundamental to  both
          actuation and  sensing, means solving an integral-differential  equation and
          this can only be  done by  means of numerical  methods. This electrostatic
          transduction principle  will  briefly be  discussed in  the  following,  together
          with a numerical example illustrating the calculation procedure.
              When applying external charges on the microcantilever and the pad that
          are equal and opposite in sign,  the  compliant  microcantilever  will be
          attracted by the  fixed pad and  will  bend  towards it.  In  doing so, the gap
          between the two parts will vary along the overlapping length   according to
          the quasistatic equilibrium between actuation forces and elastic properties of
          the microcantilever. Thus, the posed problem is not purely an actuation one,
          as  the elastic  features of the microcantilever condition  the entire situation,
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