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                                                 Resonant Micromechanical Systems

                                                             Resonant Micromechanical Systems  245

                                    w 1
                                                                       x

                                                                               m
                                             w 2
                                   l 1                l 1
                                                                                   z

                                             l 2
                                            (a)                               (b)

                              Figure 5.20 Torsion paddle microbridge: (a) geometry; (b) simplified model with degrees
                              of freedom.

                              these values and the ranges allotted to the nondimensional parameters
                              c l  and  c w , Fig. 5.19  indicates that the torsional  resonant frequency
                              predicted by model I is smaller than that produced by model III.

                              5.2.3  Other examples of beam-type
                              microresonators
                              Several other examples of microresonators are discussed next that are
                              designed by using relatively large segments which can be considered
                              rigid, connected to smaller components which are flexible. As a conse-
                              quence, all following resonators will be qualified according to the as-
                              sumptions of model I, where the inertia fraction was only produced by
                              the massive segment whereas the stiffness was given by the relatively
                              smaller compliant segments.
                                Example: Analyze the torsional resonant frequency of the torsional bridge
                                sketched in Fig. 5.20a and compare it to the corresponding resonant fre-
                                quency of the regular bridge design illustrated in Fig. 4.19.
                                                                           1
                                  The design of Fig. 5.20a is analyzed by Xiao et al.  as an electrostatic tor-
                                                                      2
                                sional actuator and by Selvakumar and Najafi  as a microaccelerometer, but
                                it can also be utilized as a torsional resonator for mass addition detection
                                purposes—the subject of mass addition detection is studied more thoroughly
                                in Chap. 6. The assumption made here is that the central segment is rigid
                                (and possesses a mass m, as indicated in Fig. 5.20b), whereas the identical
                                root segments are compliant and are considerably lighter than the middle
                                segment such that their inertia contribution can be neglected.
                                  Compared to the paddle microbridge of Fig. 4.19, the design sketched in
                                Fig. 5.20a is quite similar except for the middle segment which is placed asym-
                                metrically with respect to the longitudinal axis of the hinges. Figure 5.20b
                                indicates the main possible motions (degrees of freedom) which are
                                the rotation around the x axis (implying torsion of the root segments) and




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