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8.3 Micromachined Gyroscopes                                                  197

            Table 8.3  (Continued)
                               Single axis (20G,  Analog output; bandwidth 0 to 700 Hz;
                               50G), K-Beam  noise floor 7 µG/√Hz (20G), 12 µG/√Hz
                               range      (50G); resolution 100, 170 µG; sensitivity
                                          100, 60 mV/G, supply voltage 15V to 28V,
                                          bulk-micromachined sensing element
                               Single axis (2G),  Analog output; bandwidth 0 to 2 kHz;  Employs analog electrostatic feedback.
                               ServoK-Beam  noise floor 0.8 µG/√Hz; resolution 2.5G;
                                          sensitivity 1.5 V/G; supply voltage 6V to
                                          15V; bulk-micromachined sensing element
            Motorola           Single axis (1.5G  Ratiometric output; bandwidth from 50 to  Appr. cost: $8
            (http://www.motorola.com)  to 250G)  400 Hz; noise floor 110 G/vHz; sensitivity
                               Dual axis (38G)  from 1.2 V/G (1.5G) to 8 mV/G (250G);
                                          supply voltage 5V; surface-micromachined
                                          sensing element
                                          Bandwidth 400 Hz; sensitivity 50 mV/G
            Sensornor          Single axis (50G,  Ratiometric analog output; bandwidth 400  Piezoresistive detection, for airbag
            (http://sensornor.com)  100G, 250G)  Hz; sensitivity 20 mV/G; supply voltage  applications
                                          5V to 11V
                               Dual axis (50G)  Ratiometric analog output; bandwidth 400
                                          Hz; resolution 0.02G; sensitivity 40 mV/G;
                                          supply voltage 5V; bulk-micromachined
                                          sensing element
            STMicroelectronics  Dual axis (2G,  Analog output; bandwidth 0 to 4 kHz;  For handheld gamepad devices
            (http://st.com)    6G)        noise floor 50 µG/√Hz; sensitivity 1 V/G;
                                          supply voltage 5V






                  velocity υ increases with the distance of the ball from the center (v = rΩ), but any
                           ang                                                ang
                  change in velocity inevitably gives rise to acceleration in the same direction.
                      This acceleration is given by the cross product of the angular velocity Ω of the
                  disk and the radial velocity v of the ball:
                                             r
                                     →     →→                 →       →→
                   Coriolis acceleration: a =2Ω ×ν  r ;  Coriolis force: F =2mΩ ×ν  r
                                                                c
                                      c
                      Macroscopic mechanical gyroscopes typically use a flywheel that has a high
                  mass and spin speed and hence a large angular momentum which counteracts all
                  external torque and creates an inertial reference frame that keeps the orientation of
                  the spin axis constant. This approach is not very suitable for a micromachined



                                                        v r


                                                           v ang  = r Ω
                                                           a Cor  = 2v x Ω
                                                                 r

                                                       Ω









                  Figure 8.21  A ball rolling from the center of a spinning disk is subjected to Coriolis acceleration
                  and hence shows a curved trajectory.
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