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232                                                                    Flow Sensors

                 membrane is loaded with the flow’s static pressure p . The pressure difference
                                                                   stat
                 between p and p   causes a deflection of the membrane, which changes the capaci-
                          tot    stat
                 tance between the electrodes (Figure 9.23). A reference capacitor is located around
                 the perimeter of the membrane to compensate for the dielectric coefficient of the
                 fluid between the capacitor electrodes.
                    The advantage of the differential pressure flow measuring principle is that the
                 heating of the fluid is negligible. This can be important when using temperature-
                 sensitive fluids or during chemical reactions.
                    A disadvantage of differential pressure flow sensors is that they are affected by
                 particles because of the necessary flow restrictions. Also, the total pressure loss
                 might be a problem if, for example, a micropump is used that can only pump against
                 a certain backpressure. Temperature changes can have strong influences on the sens-
                 ing signal due to the change in density and viscosity. Therefore, the temperature
                 must also be monitored. The differential pressure sensing principle is better suited
                 for liquids as the compressibility of gases distorts the measurement results. Data for
                 pressure difference type flow sensors are listed in Table 9.4.


          9.4   Force Transfer Flow Sensors


                 9.4.1  Drag Force
                 This type of flow sensor consists of a cantilever beam, or paddle, with an integrated
                 strain gauge resistor. When the cantilever is immersed in a flowing fluid, a drag force
                 is exerted resulting in a deflection of the cantilever, which can be detected by the pie-
                 zoresistive elements incorporated in the beam. The figures in the following sections
                 show schematics of devices using this measurement principle.





                                                 Upper capacitor        Pyrex
                                                 electrode              glass
                                      Fluid
                                      passage



                                                                Silicon  Thin silicon
                                                                boss     membrane
                                                 Lower capacitor
                                                 electrode

                                                          p tot        p stat



                            Fluid flow


                                                                     p stat
                                                              Boss
                                                              deflection
                 Figure 9.23  Schematic of a micromachined flow sensor based on the Prandtl tube. The fluid
                 passage is 250 µm wide. The gap between the capacitor electrodes is 8 µm and the membrane
                 thickness is 14 µm. (After: [87].)
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