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5.6 Actuation Techniques                                                      107

                  5.6.2 Piezoelectric

                  As we have already seen, piezoelectric devices can be used for both sensor and
                  actuator applications. An applied voltage across the electrodes of a piezoelectric
                  material will result in a deformation that is proportional to the magnitude of the
                  voltage (strictly electric field). The displacement across a bulk sample of PZT with
                  an actuation voltage of several hundred volts, for example, is only a small fraction
                  of a micron. When such a system is scaled down to that of a typical MEMS actuator,
                  a displacement of several orders of magnitude less is obtained! For this reason, some
                  form of mechanical amplification is needed in order to generate useful displace-
                  ments. Such a device can be fabricated by depositing a piezoelectric film onto a sub-
                  strate in the form of a cantilever beam as shown in Figure 5.16. This type of
                  structure is referred to as a piezoelectric unimorph. The deflection at the free end of
                  the beam is greater than that produced in the film itself.
                      Piezoelectric actuators are often used in micropumps (see Chapter 9) as a way of
                  deflecting a thin membrane, which in turn alters the volume within a chamber
                  below. Such a structure is depicted in Figure 5.17. The device comprises two silicon
                  wafers bonded together. The lower wafer comprises an inlet and outlet port, which
                  have been fabricated using bulk micromachining techniques. The upper wafer has
                  been etched to form the pump chamber. The shape of the ports gives rise to a prefer-
                  ential direction for the fluid flow, although there is a degree of flow in the reverse
                  direction during pumping. So the ports behave in a similar manner to valves. An
                  alternative structure comprises cantilever-type flaps across the ports, but these often
                  suffer from stiction during pumping. When a voltage is applied to the piezoelectric
                  material, this results in a deformation of the thin membrane and hence changes the
                  volume within the chamber. This is depicted in Figure 5.17(b). Typical flow rates
                  are in the range of nanoliters to microliters per minute, depending on the dimension
                  of the micropump.


                  5.6.3  Thermal

                  Thermal actuation techniques tend to consume more power than electrostatic or
                  piezoelectric methods, but the forces generated are also greater. One of the basic


                                                      Piezoelectric material
                                       Pump chamber

                                        Si
                                        Si
                                                     (a)


                                         Si
                                         Si
                                                 Out           In
                                                     (b)
                  Figure 5.17  A simple micropump with a piezoelectric actuator: (a) the situation with no applied
                  voltage; and (b) the effect of applying a voltage to the piezoelectric layer.
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