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                                          Microbridges: Lumped-Parameter Modeling and Design

                                               Microbridges: Lumped-Parameter Modeling and Design  199
                              of the equivalent (effective) mass to the kinetic energy of the vibrating
                              microcantilever such that

                                                   l 1                l +l 2
                                                                      1
                                                  œ  f (x) w(x) dx + w  œ  f (x) dx
                                                        2
                                                                            2
                                                    b
                                                                         b
                                                  0                  l 1
                                        m b,e  = ȡt                                     (4.110)
                                                      2l +l 2
                                                       1
                                                     œ    f (x) w(x) dx
                                                              2
                                                  +       b
                                                      l +l
                                                      1  2
                              Due to the transverse symmetry of the microbridge shown in Fig. 4.18,
                              Eq. (4.110) can also be expressed as
                                                  l 1                l +l 2
                                                                     1
                                                 œ
                                                                            2
                                                       2
                                        m   = ȡt 2 f (x) w(x) dx + w  œ  f (x) dx       (4.111)
                                         b,e        b                   b
                                                  0                  l 1
                              A check is performed again to see whether the generic Eq. (4.111) re-
                              duces to the known mass equation in the case where the two end seg-
                              ments of the microbridge are identical to the middle one. Indeed, when
                              l 1  = l 2  = l/3 and w(x) = w, Eq. (4.111) reduces to Eq. (4.12), which gives
                              the effective mass of a constant rectangular cross-section microbridge
                              of length l and cross section defined by w and t.
                                By combining Eqs. (4.101) with Eq. (4.111), the resonant frequency
                              corresponding  to  bending  vibrations  of  the  microbridge  sketched  in
                              Fig. 4.18 is

                                                               1
                                 Ȧ   =
                                  b,e          l                 l + l
                                              œ  1   2            1  2    2
                                          ȡ t 2. f (x) w(x) dx + w.   f (x) dx
                                                 b
                                                                       b
                                               0                 œ l 1                  (4.112)
                                                                                    2 ƍ
                                                                     2
                                                           ƍ
                                                               2 ƍ
                                                                        ƍ
                                                  ƍ
                                                                       ƍ
                                                2
                                                                                 ƍ
                                                                                ƍ
                                         × c + c C í 2c c C + c C + c C í 2c c C + c C  ƍ
                                                                                    4 l
                                                                            3 4 c
                                                                     3 r
                                                2 r
                                                       1 2 c
                                                               1 l
                              For a microbridge formed of three identical segments (l 1  = l 2  = l/3) of
                              constant rectangular cross section, the generic Eq. (4.112) reduces to
                              Eq. (4.13), which defines the bending resonant frequency of a constant-
                              cross-section microbridge of length l.
                              Torsional resonant frequency. In torsion, the lumped-parameter stiffness
                              being  associated  with  the  midspan  of  the  microbridge  pictured  in
                              Fig.  4.18  is  determined  by  first  calculating  the  endpoint  reaction
                              moment produced by a torsional moment (about the x axis) applied at
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