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222                                                         Chapter 4
         the interaction  with an  external electromagnetic  field, as  suggested by
         Kruusing and Mikli  [9] for instance. Figure 4.39 shows four different cases
         of  magnetization m of  a  microcantilever that  is  placed in  an  external
         electromagnetic field B,  whose direction  is assumed to  be  constant. The
         interaction  between  the   magnetization  vector  and  the   external
         electromagnetic field vector B results in a force and a moment that act on the
         cantilever and which are figuratively shown in Figs. 4.39 (a) through (d). The
         force and the moment are calculated as:








         It can be seen that in the case where the electromagnetic field B varies about
         the z-direction, a force  will be produced about the same direction, and will
         bend the microcantilever,  irrespective of the direction of magnetization.  The
         moment, however,  according to  the  definition of  Eq.  (4.91)  will  have
         different directions, as a function of the magnetization direction. In the case
         of Fig. 4.39 (b), the total moment will be a pure bending moment combining
         to the bending effect produced by the force   whereas Fig. 4.39 (c) depicts
          the situation where the moment is a torsional  one. When m has an arbitrary
          direction, as  shown in  Fig.  4.39 (d), the  resulting  moment can  be  resolved
          into a bending component and a torsion component.

          Example 4.10
             A microcantilever of length l and cross-sectional dimensions w and t is
          magnetized about a direction  as  shown in Fig. 4.39 (d). The microdevice is
          used to monitor a constant  external  field  B, as sketched in the  same figure.
          An optical system can measure a maximum slope    at  the  microcantilever
          tip. What is the maximum value of the magnetic field that can be detected by
          this sensing microsystem ?

          Solution
             There will be no force acting at the free end, because the external field is
          assumed constant. The  moment produced at that end can  be  resolved into  a
          torsional component and a bending one. The later one has the expression:





          The tip slope can be found as:





          By combining Eqs. (4.92) and (4.93) results in:
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