Page 103 - An Introduction to Microelectromechanical Systems Engineering
P. 103

82                      MEM Structures and Systems in Industrial and Automotive Applications

                 designs. Measuring the change in resistance and amplifying the corresponding out-
                 put signal tend to be rather simple, requiring a basic knowledge of analog circuit
                 design. A drawback of silicon piezoresistivity is its strong dependence on tempera-
                 ture which must be compensated for with external electronics.
                    By contrast, capacitive sensing relies on an external physical parameter changing
                 either the spacing or the relative dielectric constant between the two plates of a
                 capacitor. For instance, an applied acceleration pushes one plate closer to the other.
                 Or in the example of relative humidity sensors, the dielectric is an organic material
                 whose permittivity is function of moisture content [1]. The advantages of capacitive
                 sensing are very low power consumption and relative stability with temperature.
                 Additionally, the approach offers the possibility of electrostatic actuation to perform
                 closed-loop feedback. The following section on actuation methods explains this
                 point further. Naturally, capacitive sensing requires external electronics to convert
                 minute changes in capacitance into an output voltage. Unlike measuring resistance,
                 these circuits can be substantially intricate if the change in capacitance is too small.
                 This is frequently the case in MEMS where capacitance values are on the order of 1
                 pF (10 −12  F) and changes in capacitance can be as small as a few fF (10 −15  F).
                    Yet another sensing approach utilizes electromagnetic signals to detect and
                 measure a physical parameter. Magnetoresistive sensors on the read heads of high-
                 density computer disk drives measure the change in conductivity of a material slab in
                 response to the magnetic field of the storage bit. In Hall-effect devices, a magnetic
                 field induces a voltage in a direction orthogonal to current flow [2]. Hall-effect sen-
                 sors are extremely inexpensive to manufacture. They are used in high-reliability
                 computer keyboards and make excellent candidates to measure wheel velocity in
                 vehicles. Another form of electromagnetic transducing uses Faraday’s law to detect
                 the motion of a current-carrying conductor through a magnetic field. Two yaw-rate
                 sensors described later in this chapter make use of this phenomenon. The control
                 electronics for magnetic sensors can be readily implemented using modern CMOS
                 technology, but generating magnetic fields often necessitates the presence of a per-
                 manent magnet or a solenoid.


                 Common Actuation Methods
                 A complete shift in paradigm becomes necessary to think of actuation on a miniature
                 scale—a four-stroke engine is not scalable. The next five schemes illustrate the diver-
                 sity and the myriad of actuation options available in MEMS. They are electrostatic,
                 piezoelectric, thermal, magnetic, and phase recovery using shape-memory alloys.
                 The choice of actuation depends on the nature of the application, ease of integration
                 with the fabrication process, the specifics of the system around it, and economic jus-
                 tification (see Table 4.2). Examples of each actuation method will arise throughout
                 this chapter and the next.


                 Electrostatic actuation
                 Electrostatic actuation relies on the attractive force between two conductive plates
                 or elements carrying opposite charges. A moment of thought quickly reveals that the
                 charges on two objects with an externally applied potential between them can only
                 be of opposite polarities. Therefore, an applied voltage, regardless of its polarity,
   98   99   100   101   102   103   104   105   106   107   108