Page 82 - Mechanical Engineers' Handbook (Volume 2)
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2 Flexural Devices in Measurement Systems  71

                           tube is typically used to modify the alternating current (ac) impedance of bridge transducers.
                           Bourdon tubes can be integrated into transducers to achieve extremely high accuracies and
                           have been manufactured from perfectly elastic materials such as quartz.
                              Transducers employing Bourdon tubes tend to be physically large and easily damaged
                           by environmental inputs such as acceleration. In addition, the tubes themselves afford poor
                           frequency response to time-varying pressure.


            2.3 Clamped Diaphragms
                           Clamped diaphragms are another flexure used to transform a measurand into a strain or
                           displacement proportional to applied pressure. A small, flat, circular diaphragm can be made
                           simply, and it can be placed flush against surfaces whose flow dynamics are being studied.
                           This type of diaphragm is typically designed to deflect in accord with theory associated with
                           clamped circular plates. Corrugated diaphragms provide extensibility over a greater linear
                           operating range than do flat diaphragms. A catenary diaphragm consists of a flexurally weak
                           seal diaphragm bearing against a thin cylinder whose motion is measured. The compliance
                           of a flat, clamped circular diaphragm is defined as
                                                                    2
                                                              4
                                                        y   3R (1     )
                                                              0
                                                                                                 (2)
                                                                 3
                                                        P      16tE
                           where y is the deflection of the center of the diaphragm, P is the applied pressure, R is the
                                                                                             0
                           diaphragm radius,   is Poisson’s ratio, t is the diaphragm thickness, and E is the modulus
                           of elasticity of the diaphragm material. Somewhat analogous to the cantilever beam, a com-
                           pliant diaphragm will have a large radius, be thin, and be made of a low-modulus material.
                           Equation (2) holds for deflections no greater than t.
                              Figure 1 shows the radial and tangential strain distribution in a flat, clamped, circular
                           diaphragm. The radial and tangential strains at the center of the diaphragm are identical.
                           The tangential strain decreases to zero at the periphery while the radial strain becomes
                           negative. Figure 2 describes a strain gage pattern designed to take advantage of this strain
                           distribution. The central sensing elements measure the higher tangential strain while the
                           radial sensing elements measure the high radial strains near the periphery. Resistance strain
                           gages are discussed beginning in Section 3.




















                           Figure 1 Radial and tangential strain distribution in a flat, clamped, circular diaphragm. (Courtesy of
                           Measurements Group, Inc., Raleigh, NC.)
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