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                                         Microcantilever and Microbridge Systems for Mass Detection

                                          Microcantilever and Microbridge Systems for Mass Detection  309
                                                                                          z
                              deposited                                        l p    l 1
                                            l p   l 1
                                layer
                                                                                F 2z
                                                   l s
                                                                          q z         F 1z  M 1y
                                                          deflection  sensing
                                   microcantilever               x     5    4      3  2  l s 1
                                            l                                   l


                                             (a)                                (b)
                              Figure 6.16  Layer-mass detection by constant rectangular cross-section microcantilever:
                              (a) side view of setup; (b) side view of microcantilever with equivalent distributed load
                              q z  and dummy loading F 1z , M 1y , F 2z .

                              (bending) resonant frequency, can be utilized to evaluate the quantity
                              of the deposited mass, as shown in the next two subsections.

                              Static approach. Extraneous mass  can attach over a length  l p  on a
                              constant-cross-section microcantilever, as sketched in Fig. 6.16. Given
                              that  deposition is produced over the  entire  width  w (not shown in
                              Fig. 6.16), and the length of the deposited layer is l p , and this layer is
                              positioned at l s  from the free end of the microcantilever, as shown in
                              Fig. 6.16a, to determine the quantity of deposited mass ǻm requires
                              also knowledge of the lengths l l  and l p ; in other words, three experi-
                              mental quantities are necessary. There can be two deflections—u 1z  at
                              the free end and u 2z  measured at a distance l s  from the free end—as
                              well as the slope (rotation) ș 1y  at the same free end. These quantities
                              can be measured quasi-statically by means of laser interferometry, for
                              instance.
                                The situation pictured in Fig. 6.16a is equivalent to the model  of
                              Fig. 6.16b where the gravitational action of the  deposited layer  is
                              substituted by a uniformly distributed load q  acting over the length
                                                                        z
                              l p . Over this length, the bending stiffness will also be modified from the
                              original one, because the attached mass adds to the microcantilever. To
                              express the three deformations, u , ș , and u , three dummy loads
                                                              1z
                                                                 1y
                                                                          2z
                              F 1z , M 1y , and F 2z  (all equal to zero in the end) are applied at points 1
                              and  2, respectively,  also indicated in Fig. 6.16b. By  applying
                              Castigliano’s  displacement  method,  the three deformations are ex-
                              pressed as











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