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ADXL322EB Datasheet(PDF) 13 Page - Analog Devices |
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ADXL322EB Datasheet(HTML) 13 Page - Analog Devices |
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13 / 16 page ![]() ADXL322 Rev. 0 | Page 13 of 16 Peak-to-peak noise values give the best estimate of the uncer- tainty in a single measurement. Table 7 gives the typical noise output of the ADXL322 for various CX and CY values. Table 7. Filter Capacitor Selection (CX, CY) Bandwidth (Hz) CX, CY (μF) RMS Noise (mg) Peak-to-Peak Noise Estimate (mg) 10 0.47 0.9 5.3 50 0.1 2 11.8 100 0.047 2.8 16.7 500 0.01 6.2 37.3 USE WITH OPERATING VOLTAGES OTHER THAN 3 V The ADXL322 is tested and specified at VS = 3 V; however, this part can be powered with VS as low as 2.4 V or as high as 6 V. Note that some performance parameters change as the supply voltage is varied. The ADXL322 output is ratiometric, so the output sensitivity (or scale factor) varies proportionally to supply voltage. At VS = 5 V, the output sensitivity is typically 750 mV/g. At VS = 2.4 V, the output sensitivity is typically 335 mV/g. The zero g bias output is also ratiometric, so the zero g output is nominally equal to VS/2 at all supply voltages. The output noise is not ratiometric but is absolute in volts; therefore, the noise density decreases as the supply voltage increases. This is because the scale factor (mV/g) increases while the noise voltage remains constant. At VS = 5 V, the noise density is typically 150 μg/√Hz, while at VS = 2.4 V, the noise density is typically 300 μg/√Hz, Self-test response in g is roughly proportional to the square of the supply voltage. However, when ratiometricity of sensitivity is factored in with supply voltage, the self-test response in volts is roughly proportional to the cube of the supply voltage. For example, at VS = 5 V, the self-test response for the ADXL322 is approximately 610 mV. At VS = 2.4 V, the self-test response is approximately 59 mV. The supply current decreases as the supply voltage decreases. Typical current consumption at VS = 5 V is 700 μA, and typical current consumption at VS = 2.4 V is 340 μA. USE AS A DUAL-AXIS TILT SENSOR Tilt measurement is one of the ADXL322’s most popular applications. An accelerometer uses the force of gravity as an input vector to determine the orientation of an object in space. An accelerometer is most sensitive to tilt when its sensitive axis is perpendicular to the force of gravity (that is, when the pack- age is parallel to the earth’s surface). At this orientation, the accelerometer’s sensitivity to changes in tilt is highest. When the accelerometer is oriented on axis to gravity (near its +1 g or −1 g reading), the change in output acceleration per degree of tilt is negligible. When the accelerometer is perpendicular to gravity, its output changes nearly 17.5 mg per degree of tilt. At 45°, its output changes at only 12.2 mg per degree of tilt, and resolution declines. Converting Acceleration to Tilt When the accelerometer is oriented so both its X-axis and Y-axis are parallel to the earth’s surface, it can be used as a 2-axis tilt sensor with both a roll axis and a pitch axis. Once the output signal from the accelerometer has been converted to an acceleration that varies between −1 g and +1 g, the output tilt in degrees is calculated as PITCH = ASIN(AX/1 g) ROLL = ASIN(AY/1 g) Be sure to account for overranges. It is possible for the accelerometers to output a signal greater than ±1 g due to vibration, shock, or other accelerations. |
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