Page 16 - Mechanical design of microresonators _ modeling and applications
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                                            Design at Resonance of Mechanical Microsystems

                                                   Design at Resonance of Mechanical Microsystems  15

                                                       l x



                                                v            movable plate


                                          y 0

                                                 fixed plate




                              Figure 1.13 Slide-film flow in the fluid surrounding a movable plate–fixed plate couple
                              (top view).

                              corresponding to the fluid damping generated through the relative mo-
                              tion on the side faces between two comb fingers is
                                                           ʌ 2 ȝ
                                                    Q C,s  =  Ȟ                          (1.47)
                                                           Ȧ
                                                               y
                                                                0
                              where the subscript s points to the side region of the conjugate plates.
                                Stokes-type flow is responsible for damping produced both above and
                              underneath the movable plate shown in Fig. 1.12. The turbulent Stokes
                              flow which extends over the penetration height į is characterized by the
                              quality factor
                                                            ʌ 2 ȝ
                                                    Q S,a  =  Ȧ  Ȟ  į                    (1.48)

                                                               10
                              According to Cho, Pisano, and Howe,  the Stokes flow damping under-
                              neath the moving plate is
                                                          ʌ 2 ȝ
                                                  Q S,u  =  Ȧ  Ȟ  į  f (ȕ)               (1.49)

                                                   sinh(2ȕz ) +sin(2ȕz )
                                                                    0
                                                          0
                              where         f (ȕ) =                                      (1.50)
                                                   cosh(2ȕz ) ෹ cos(2ȕz )
                                                          0         0
                              and
                                                            1
                                                        ȕ =                              (1.51)
                                                            į






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