Page 280 - Mechanical design of microresonators _ modeling and applications
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                                                 Resonant Micromechanical Systems

                                                             Resonant Micromechanical Systems  279



















                                    (a)                           (b)
                              Figure 5.52 Modes in a vibratory ring gyroscope: (a) primary (drive) mode; (b) secondary
                              (sense) mode.

                              5.6 Tuning Forks
                              Tuning forks have long been used as standard pitch tools for musical
                              instrument calibration.  Another  utilization  of tuning forks is in the
                              clock and wristwatch industry as frequency standards. Resonating
                              tuning forks, such as the ones introduced in Chap. 1, can also be em-
                              ployed as microsensors in a similar manner to gyroscopes in detecting
                              changes in an external angular velocity, as shown by Satoh, Ohnishi,
                                             23
                                                                            24
                                                                                         25
                              and Tomikawa;  Sato,  Ono, and  Tomikawa;  Momosaki;  or
                                      26
                              Matsiev.  The tuning forks operate similarly to gyroscopes, and the
                              Coriolis effects are again the underlying principle. The classical tuning
                              fork sensor is sketched in Fig. 5.53, where two variants are outlined. In
                              the first variant, the driving is out-of-the-plane, which results in Cori-
                              olis accelerations  pulling  away the two tines in  their plane
                              (Fig. 5.53a). In the second variant (Fig. 5.53b), driving and sensing in-
                              terchange, with the net result that the two tines are deformed out-of-
                              the-plane through Coriolis effects.
                                The vibrational amounts involved in one tine of the tuning fork are
                              sketched in Fig. 5.54. The input  to  the tine consists  of the angular
                              velocity Ȧ which is applied about the z axis. A sinusoidal force is driving
                              the tine about the x axis, and the result is a relative velocity v  of the
                                                                                        r
                              tip of the tine about the same axis. The interaction between the angular
                              velocity and relative  velocity results in  a Coriolis-type  acceleration
                              about the y direction.
                                By ignoring the damping, the dynamic equations of motion about the
                              drive (x) and sense (y) axes can be written, using a lumped-parameter
                              model, as follows:





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