Page 111 - MEMS Mechanical Sensors
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100                                                Mechanical Transduction Techniques



                                   a max

                                                                    3dB


                             Amplitude










                                                        f 1  f 2       Frequency
                                                         f 0
                 Figure 5.10  A typical characteristic of a resonant system.



                 mechanism will be greater than that of a low-Q system. A high Q means little energy
                 is required to maintain the resonance at constant amplitude, thereby broadening the
                 range of possible drive mechanisms to include weaker techniques. A high Q-factor
                 also implies the resonant structure is well isolated from its surroundings, and there-
                 fore, the influence of external factors (e.g., vibrations) will be minimized.
                    The Q-factor can also be calculated from Figure 5.10 using

                                                   f
                                               Q =  0                                 (5.21)
                                                   ∆ f

                 where resonant frequency f corresponds with a , the maximum amplitude, and ∆f
                                                           max
                                         0
                 is the difference between frequencies f and f . Frequencies f and f correspond to
                                                          2
                                                    1
                                                                             2
                                                                       1
                 amplitudes of vibration 3 dB lower than a .
                                                       max
                    The Q-factor is limited by the various mechanisms by which energy is lost from
                 the resonator. These damping mechanisms arise from three sources:
                    1. The energy lost to a surrounding fluid (1/Q );
                                                               a
                    2. The energy coupled through the resonator’s supports to a surrounding solid
                       (1/Q );
                            s
                    3. The energy dissipated internally within the resonator’s material (1/Q).
                                                                                     i
                    Minimizing these effects will maximize the Q-factor as shown here:

                                          1    1    1    1
                                            =    +    +                               (5.22)
                                          Q   Q    Q    Q
                                                a    s    i
                    Energy losses associated with 1/Q are potentially the largest, and therefore the
                                                   a
                 most important, of the loss mechanisms. These losses occur due to the interactions
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