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                                   Microhinges and Microcantilevers: Lumped-Parameter Modeling and Design

                              150   Chapter Three
                              3.5 Sandwiched Microcantilevers
                              (Multimorphs)
                              Sandwiched components such as microcantilevers or microbridges are
                              often utilized in microtransduction (actuation and/or sensing) where
                              one layer achieves the structural and elastic recovery functions (most
                              often the silicon or polysilicon) and the other layers are active in the
                              sense that they deform under activation or environmental stimuli. The
                              resonant frequencies corresponding to axial deformation, torsion, and
                              loading are presented next for equal-length microcomponents and for
                              dissimilar-length ones.

                              3.5.1  Microcantilevers of equal-length
                              layers
                              In  equal-length  multimorphs,  the  component  layers  have  identical
                              lengths. Figure 3.29 shows a microcantilever consisting of n layers. The
                              resonant frequencies are determined next for this micromember. The
                              resonant frequencies for a multimporph are very similar to those of a
                              homogeneous micromember having the same length.
                                In the case of axial vibrations, for instance, an equivalent rigidity
                                                                                5
                              needs to be used in the form (see Lobontiu and Garcia ):
                                                          n  E A
                                                    k a,e  = ™  i  i                    (3.128)
                                                         i =1  l
                              where l  is  the  identical  length  and  A   is  the  cross-sectional  area  of
                                                                  i
                              the ith  component.  In  a  similar  manner,  it  can  be  shown  that  the
                              lumped-parameter  mass  which  needs  to  be  placed  at  the
                              microcantilever’s free tip, in order to generate the same inertial effect
                              as  the  distributed  mass  of  the  multimorph,  according  to  Rayleigh’s
                              principle, is



                                                 layer # n     layer # i   layer # 1









                                                               l
                              Figure 3.29 Sandwiched microcantilever.




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