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                                          Microbridges: Lumped-Parameter Modeling and Design

                              222   Chapter Four






















                              Figure 4.34  Underneath three-dimensional view of a rectangular cross-section micro-
                              bridge network.


                              properties are identical to those of the similar microbridge of Fig. 4.28
                              which are expressed in Eqs. (4.168) through (4.174).


                              4.5 Resonator Microbridge Arrays
                              Several microbridges having identical rectangular cross sections can be
                              used in the same construction as a means of sensing a frequency range
                              through resonance. Figure 4.34 shows such an assembly formed of sev-
                              eral dissimilar-length microbridges.
                                The idea is to use a network of microbridges and microcantilevers
                              which  will resonantly cover  a certain frequency range (the audible
                              domain, from 20 to 20,000 Hz, for instance), as shown in the sketch of
                              Fig. 4.34. Different sound pressures and  frequencies will  excite
                              different resonant  frequencies, and therefore one specific beam will
                              resonate at a given input. It is thus possible to cover the entire audible
                              range.
                                It can be shown that the bending resonant frequency of a fixed-fixed
                              beam (bridge) is calculated as

                                                              t 4  E
                                                      l =1.014                          (4.179)
                                                               f  ˮ
                              Figure 4.35 plots this length for the audible range (up to 20,000 Hz), in
                                                                                      3
                              the case of polysilicon beams with E = 165 GPa, ȡ = 2300 kg/m , and for
                              an average thickness of t = 500 nm, and this length profile should be
                              identical to the geometric envelope shown in Fig. 4.34.





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