Comparison of Different Accelerometer Types

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Comparison of different accelerometer types. Parameter Piezo-electric Piezoresistive Silicon Piezoresistive Thick film Capacitive DC response No Yes Yes Yes Bandwidth Wide Moderate Low Wide Self-generating Yes No No No Impedance High Low Low Very High Signal level High Low Low Moderate Temperature range (oC) -55-100 -55-150 -50-120 -200-200 Linearity Good Moderate Moderate Excellent Static Calibration No Yes Yes Yes Cost High Low Low High Ruggedness Good Moderate Moderate Good Suitable for shock Yes No No No *Expects could change for special designs. Accelerometers There are many types of accelerometers, which sense the motion of a mass in order to measure acceleration. There are many different ways to detect the motion. Moreover, there are many parameters to consider such as sensitivity or susceptibility to interference and bandwidth. Therefore, it is important to know which type of sensor to use in order to obtain the best performance in the application. The types of accelerometers are: Piezoelectric (PE), Piezoresistive (PR) and Capacitive. Piezoelectric accelerometers. Piezoelectric accelerometers are made of two parts. The mass, which produces a force due to the acceleration, and the piezoelectric transducer, which generates a charge due to the mass force applied. In the most common design, the mass is between some piezoelectric discs. The mass applies a force on the piezoelectric when it oscillates on it axis. The piezoelectric develops a variable charge in proportion of the force exerted by the mass. Fig 9.5 page 157 A piezoelectric generates an electrical charge when it is pressed. There are some natural piezoelectric materials such as quartz and Rochelle salt, but the charge produce is very small.... ... middle of paper ... ...he length difference is dl, which is the result from the length after minus the length before a force was applied. However, the width and the thickness decreases and it can be noted as dw and dt. This phenomena is due to Poisson’s ratio v, where dw = -vwε and dt = -vtε. Figure 9.7. The reaction of a piezoresistors when a force is applied. The variable use before are useful in order to calculate the cross-sectional area A’, which is: A’ = (W – dw)(t - dt) = wt + 2vwtε + v2wtε . The value of v2wte is smaller than the other two values, thus it could be disregarded. Therefore, the equation could be A - A’ = dA = -2vεA → -2vε = dA/A → dR/R = dρ/ρ + dl/l - dA/A So the gauge factor k is K = ((dρ /ρ )/ ε) + (1 + 2v) Usually v is around 0.2 and 0.3. The last equation presents that the resistivity and geometry are factors that affect the longitudinal gauge facto.

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