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XMMA2000W Datasheet(PDF) 5 Page - Motorola, Inc |
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XMMA2000W Datasheet(HTML) 5 Page - Motorola, Inc |
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5 / 8 page ![]() XMMA1000P XMMA2000W 5 Motorola Sensor Device Data PRINCIPLE OF OPERATION The Motorola accelerometer is a surface–micromachined integrated–circuit accelerometer. The device consists of a surface micromachined capaci- tive sensing cell (G–cell) and a CMOS signal conditioning ASIC contained in a single integrated circuit package. The sensing element is sealed hermetically at the wafer level using a bulk micromachined “cap’’ wafer. The G–Cell is a mechanical structure formed from semi- conductor materials (polysilicon) using semiconductor pro- cesses (masking and etching). It consists of two stationary plates with a moveable plate in–between. The center plate can be deflected from its rest position by subjecting the sys- tem to an acceleration (Figure 1). When the center plate deflects, the distance from it to one fixed plate will increase by the same amount that the dis- tance to the other plate decreases. The change in distance is a measure of acceleration. The G–Cell plates form two back–to–back capacitors (Figure 2). As the center plate moves with acceleration, the distance between the plates changes and each capacitor’s value will change, (C = A ε/D). Where A is the area of the plate, ε is the dielectric constant, and D is the distance between the plates. The CMOS ASIC uses switched capacitor techniques to measure the G–Cell capacitors and extract the acceleration data from the difference between the two capacitors. The ASIC also signal conditions and filters (switched capacitor) the signal, providing a high level output voltage that is ratio- metric and proportional to acceleration. Acceleration Figure 1. Figure 2. SPECIAL FEATURES Filtering The Motorola accelerometers contain an onboard 4–pole switched capacitor filter. A Bessel implementation is used because it provides a maximally flat delay response (linear phase) thus preserving pulse shape integrity. Because the fil- ter is realized using switched capacitor techniques, there is no requirement for external passive components (resistors and capacitors) to set the cut–off frequency. Noise Calculation The noise for the Motorola accelerometer is specified as an rms value which is a statistical value of a gaussian noise source. To convert the rms values to a peak to peak value at a particular confidence level refer to Table 1. A sample cal- culation at a 99.9% confidence level is shown. Table 1. Nominal Peak to Peak Value % Confidence Level 2.0 rms 68% 3.0 rms 87% 4.0 rms 95.40% 5.0 rms 98.80% 6.0 rms 99.73% 6.6 rms 99.90% Noise rms = 3.5mVrms Noise peak to peak at a 99.9% confidence level: 3.5mVrms* 6.6 = 23.1mVpp Self–Test XMMA sensors provide a self–test feature that allows the verification of the mechanical and electrical integrity of the accelerometer at any time before or after installation. This feature is critical in applications such as automotive airbag systems where system integrity must be ensured over the life of the vehicle. A fourth “plate’’ is used in the g–cell as a self– test plate. This plate is fixed and is located under an ex- tended portion of the center (moveable) plate. When the user applies a logic high input to the self–test pin, a calibrated po- tential is applied across the self–test plate and the moveable plate. The resulting electrostatic force (Fe = 1/2 AV2/d2) causes the center plate to deflect. The resultant deflection, is measured by the accelerometer’s control ASIC and a propor- tional output voltage results. This procedure assures that both the mechanical (g–cell) and electronic sections of the sensor are functioning. Ratiometricity The XMMA1000P and XMMA2000W are designed to be “ratiometric’’. That is, their transfer function will be propor- tional to the applied supply voltage. This feature allows easy interfacing to common microcontrollers that use ratiometric A/D converters for system cost benefits. In operation, a ratiometric sensor’s gain or “sensitivity’’ will change 1:1 with applied supply voltage and the zero signal output will be at midsupply. (2.5 V for a 5 V VDD and 2.625 V for a 5.25 VDD). Minimum G Range Calculation To calculate the minimum g range values of an accelerom- eter several factors have to be taken into consideration. These considerations include, the supply voltage, the device’s sensitivity, offset voltage and output rail. A sample calculation for the minimum g range is shown below. To complete the calculation the rail and offset voltages must be subtracted from the supply voltage, then divided by the supply voltage multiplied by the device’s worst case (highest) sensitivity. V DD * 0.56VDD * 0.3V V DD(8.64mV V g) + 0.44V DD * 0.3V V DD(0.00864) + 50.93 * 34.72 V DD g Using the standard five volt power supply, the minimum g range is calculated to be: 50.926 * 34.722 5.00 + 43.98 [ 44g |
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