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                                         Microcantilever and Microbridge Systems for Mass Detection

                              304   Chapter Six
                                                                  deposited particle   y
                                                       z
                                              F z
                                    3
                                                       1                               l y
                              x                2   l x      x
                                             l
                                                                     microcantilever
                                            (a)                          (b)
                              Figure 6.11  Point-mass detection by constant-cross-section microcantilever: (a) side view;
                              (b) top view.

                              either case to evaluate the deposited mass, as two approaches can be
                              pursued, namely, the  static (quasi-static) procedure and the  modal
                              (resonant) one.


                              6.3.1  Constant-cross-section
                              microcantilevers
                              Constant (usually rectangular) cross-section microcantilevers are con-
                              structively simple devices that enable mass deposition detection. This
                              section details the mass detection process by considering first that the
                              deposition occurs in a pointlike manner and then in a layer. For each
                              situation, a static approach is presented as well as a resonance-based
                              procedure.

                              Point-mass detection. Mass can deposit (attach) locally on a very small
                              area of the microcantilever, which may well be considered a point. When
                              the microcantilever is monitored quasi-statically, the deposited mass
                              might bend the member, and this deflection change can be determined
                              experimentally. In case the experiment is conducted modally, the bend-
                              ing resonant response is altered by mass deposition, and the resulting
                              resonant frequency shift enables quantification of the deposited mass.
                              Both approaches are studied in the following subsections.
                              Static approach. The problem  of static  detection of mass presence is
                              briefly discussed next. A more detailed presentation of this subject is
                                                          21
                              given by Lobontiu and Garcia.  A pointlike mass is first assumed that
                              attaches to a microcantilever, as shown in Fig. 6.11. In essence, the
                              mass quantity ǻm, as well as its position on the microcantilever (quan-
                              tified by l x  and l y ), can be determined by considering the deformations
                              produced under the action of the deposited mass gravitational effects
                              through bending and torsion at the free end, which are u 1z , ș 1y , and
                              ș 1x , and which can be measured experimentally.






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