Page 107 - MEMS Mechanical Sensors
P. 107

96                                                 Mechanical Transduction Techniques

                 5.4.3 Wavelength

                 Wavelength-based sensing relies on the source spectrum being modulated by inter-
                 action with the microsensor. Normally a source with a broad spectrum is used. The
                 light returned from the microsensor is split into spectral segments and incident on a
                 photodetector for measurement of its intensity. By a prior knowledge of the poten-
                 tial modulation mechanism present with the microsensor, one can identify the
                 measurand and its magnitude. A good example of a wavelength-based sensor is one
                 based on the gas absorption, which is highly wavelength specific according to the
                 quantity of gas present.
                    The advantage of wavelength-based sensors is that they can be made insensitive
                 to intensity variation since these affect the whole spectrum in the same way. There-
                 fore, the measurement of a nonabsorbed wavelength can be used to reference the
                 absorbed wavelength, therefore compensating for intensity variations. In addition,
                 wavelength-based sensors often lend themselves to the measurement of multiple
                 parameters since the light spectrum can be divided according to the particular wave-
                 length corresponding to the measurand of interest.



                 5.4.4  Spatial Position
                 Figure 5.8 illustrates the principle of the modulation of special position by means of
                 the movement of a microsensor. This technique is often known as triangulation.
                    This technique is simple to implement and has the advantage of immunity to
                 source intensity variations. Its resolution is less then phase-based techniques.


                 5.4.5  Frequency
                 If optical radiation at a frequency f is incident upon a body moving a velocity v, then
                 the radiation reflected from the moving body appears to have a frequency f , where
                                                                                   1
                                               f        ν 
                                          f =      ≈  f 1+                            (5.19)
                                                           
                                                     
                                          1      v      c 
                                              1−
                                                 c
                                                                   Reflective microstructure surface
                                                                   (position 2)
                                                                   Reflective microstructure surface
                                                                   (position 1)
                   Microstructure
                   displacement





                                                                    Position-sensitive detector
                    Optical source
                                                 Displacement on detector
                                                 corresponding to movement
                                                 of microstructure
                 Figure 5.8  An example of a spatial position measurement system.
   102   103   104   105   106   107   108   109   110   111   112