Page 274 - Microsensors, MEMS and Smart Devices - Gardner Varadhan and Awadelkarim
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254    MICROSENSORS

           Table  8.6  Some  mechanical characteristics  of  three  different microflexures
  Parameter             Hammock          Folded             Crab-leg
  Bending deflection y  Axial  and bending  Bending stress  Bending stress
                          stress
  Spring  constant  k y  Nonlinear  in y  Constant  and     Constant  and
                                           independent of  y  independent  of  y
  Axial  deflection x   Axial  stress  only  Axial  and bending  Axial  and bending
                                           stress             stress
  Spring  constant  k x  Stiff:  4E mA/l  Quite  stiff      Stiff


  Table  8.7  Some  important mechanical parameters  and material properties that define  the dynamic
  deflection  of microflexures

  Parameters/properties                             Nature
  Point/distributed force,  torque, stress, pressure  Load  applied/measurand
  Width,  breadth,  thickness,  length               Size  of  structure
  Young's modulus, yield strength, buckling strength,  Material properties
    Poisson's ratio, density, viscosity,  friction
  Spring  constant,  strain, mass, moment of inertia, natural  Calculable  parameters
    frequency,  damping  coefficient
  Lateral/vertical  deflection, angular deflection, resonance,  Response
    bandwidth


     Table  8.6 provides the characteristic properties of these flexures, in which their dynam-
  ical  response  is  much  more  complicated  than  that  of  a  simple  end  mass  and  is  often
  determined using computational methods, for example, a finite-element or finite-difference
  analysis.
     When  designing dynamic structures, we  need  to consider  some  additional parameters,
  which  are  listed  in Table  8.7.


  8.4.4  Mechanical  Microstmctures

  The two most important questions that now need to be asked by the designer are as follows.
  First, if these  mechanical  structures can  be made on the  micron scale  and  second,  if they
  still  follow classical  theory, for example,  the  linear theory of elasticity.
    We  know  that  microbeams,  microbridges,  and  microdiaphragms  can  all  be  made  in
  silicon using the bulk- and surface-micromicromaching  techniques,  which were described
  in Chapters  5 and 6. In fact,  a number of worked examples of the process flow to fabricate
  the following microstructures were given:
  •  A cantilever beam  made of undoped silicon  (WE 5.1)
  •  A thin cantilever  beam               (WE 5.4)

  •  A free-standing polysilicon beam      (WE 6.1)
  •  An array of thin diaphragms/membranes  (WE 5.3)
  •  A comb resonant  structure            (WE 6.7)
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