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126                                                                 Pressure Sensors

                 diaphragm pressure sensors typically requires the use of electromechanical transduc-
                 ers rather than mechanical linkages. Electromechanical effects can be used to meas-
                 ure displacement directly or to measure the stress/strain induced in the diaphragm
                 material. Therefore, it is also useful to provide an analysis of the stress distribution
                 across a pressurized diaphragm.
                    The stress distribution will vary both across the radius and through the thick-
                 ness of the diaphragm. For example, the neutral axis [shown in Figure 6.11(a)] expe-
                 riences zero stress while the maximum stress occurs at the outer faces. At any given
                 distance r from the center of the diaphragm, one face will experience tensile stress
                 while the other experiences compressive stress. There are two stress components
                 associated with a circular diaphragm: radial and tangential. The radial stress, σ ,at
                                                                                        r
                 distance r from the center of the diaphragm is given by (6.11). The maximum radial
                 stress that occurs at the diaphragm edge (r = a) is given by (6.12).

                                              2
                                          3 Pa       r  2      
                                    σ =±        3   ) ν  − 1   ) ν                  (6.11)
                                                           ( −
                                                ( +
                                     r
                                             2
                                          8  h       a  2      
                                                 3  Pa  2
                                         σ   =±       ( +  ) ν                        (6.12)
                                                       1
                                                 4  h
                                          r max     2
                                                                                 1/2
                    Radial stress is equal to zero at a value of r given by a((1 + ν )(3 + ν )) (shown in
                 Figure 6.12). This equals 0.628 if ν = 0.3.
                    The tangential stress, σ , at distance r from the center of the diaphragm is given
                                         t
                 by (6.13). The maximum tangential stress that occurs at the diaphragm center (r =0)
                 is given by (6.14).
                                             2
                                         3  Pa        r  2      
                                                           ( +
                                    σ =±       3    )   − 1    ) ν                  (6.13)
                                                ( ν+1
                                     t       2          2
                                         8  h        a          
                                                 3      Pa 2
                                                   1
                                         σ   =±   ( +  ) ν                            (6.14)
                                                 8       h
                                          t max           2
                    The inflection circle for tangential stress is removed from that of radial stress
                                               1/2
                 and is given by a((1 + ν )(3ν + 1)) . This equals 0.827 if ν = 0.3.
                    In the case of simply supported diaphragms [as shown in Figure 6.12(a)], for a
                 round diaphragm under a uniform pressure P, the deflection y at radial distance r is
                 given by (6.15). The maximum deflection occurs at the diaphragm center and,
                 assuming ν = 0.3, is given by (6.16).
                                    3 1    2 ) (  2  r  2  )5  +ν  
                                      ( −ν
                                             Pa −
                                                                   2
                                y =                         a −  r                  (6.15)
                                                              2
                                    16       Eh 3      1 +ν        
                                                 0695 Pa  4
                                                  .
                                            y =                                       (6.16)
                                             0
                                                   Eh 3
                    The deflection of a simply supported diaphragm is shown in Figure 6.12(b). The
                 radial is given by (6.17). The maximum radial stress that occurs at the diaphragm
                 center (r = 0) is given by (6.18).
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