Page 14 - Mechanics of Microelectromechanical Systems
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Chapter 1


          STIFFNESS BASICS














          1.     INTRODUCTION


              Stiffness is a fundamental qualifier of elastically-deformable mechanical
          microcomponents and micromechanisms  whose static,  modal or  dynamic
          response  need to be evaluated. This chapter gives  a brief introduction to the
          stiffness of  microeletromechanical structural components  by  outlining the
          corresponding linear, small-deformation  theory, as  well as  by  studying
          several concrete examples.  The fundamental notions of elastic  deformation,
          strain,  stress and strain energy, which are all  related to stiffness, are briefly
          outlined.  Energy methods are further presented, specifically the Castigliano’s
          theorems,  which are  utilized  herein to  derive  stiffness or  compliance
          equations.
              A six  degree-of-freedom lumped-parameter  stiffness  model is  proposed
          for the constant cross-section fixed-free straight members that are sensitive to
          bending, axial and torsion loading. A similar model is developed for curved
          members, both  thick and  thin, by explicitly  deriving the  compliance
          equations.  Composite  beams,  either sandwiched  or in serial/parallel
          configurations, are also  presented in terms  of  their  stiffnesses.  Later, the
          stiffness of  thin  plates  and  membranes is approached  and  equations are
           formulated for circular and rectangular members. Problems that are proposed
           to be solved conclude this chapter.


           2.     STIFFNESS DEFINITION

              MEMS mainly move by elastic deformation of their flexible components.
           One way  of  characterizing the static  response  of  elastic  members is by
           defining their relevant stiffnesses.  The simple example of a linear spring is
           shown in  Fig.  1.1,  where  a force is applied  by slowly  increasing  its
           magnitude from zero to a final value   over a period of time  such that the
           force is in static equilibrium with the spring force at any moment in time.
              The force necessary to extend the spring by the quantity   is calculated
           as:
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