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FXLS8964AF 数据表(PDF) 9 Page - NXP Semiconductors |
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FXLS8964AF 数据表(HTML) 9 Page - NXP Semiconductors |
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9 / 98 page ![]() NXP Semiconductors FXLS8964AF 3-Axis Low-g Accelerometer FXLS8964AF All information provided in this document is subject to legal disclaimers. © NXP B.V. 2020. All rights reserved. Objective data sheet Rev. 2 — 30 October 2020 9 / 98 9 Mechanical and electrical specifications 9.1 Definitions Sensitivity The accelerometer sensitivity, also known as scale-factor, represents the change in acceleration input corresponding to 1 LSB change in output and is typically measured in either mg/LSB or LSB/g. Zero-g offset The accelerometer zero-g offset describes the deviation of the sensor output from the ideal values when it is stationary in earth's 1 g gravitational field. With an accelerometer stationary and placed on a level, horizontal surface, the ideal output is 0 g for the X and Y axes, and 1 g for the Z-axis. The deviation of each output from the ideal value is called zero-g offset. Offset is, to some extent, a result of stress on the sensor and how well the sensor is leveled when soldered to the board. Therefore, the zero-g offset can change after mounting the sensor onto a printed circuit board or exposing it to extensive mechanical stress. For applications that require increased precision, any residual post-board mount offset may be removed using the OFF_X/Y/Z registers, or alternatively, in the host application software. Self-Test The integrated self-test function can be used to verify correct transducer and signal chain operation without the need to apply an external acceleration stimulus. When the self- test function is activated for each axis, an electrostatic actuation force is applied to the proof mass, simulating a small change in acceleration. The device's self-test function is independently exercisable for each axis, along with a selectable displacement direction (polarity). The device need not be static while exercising the self-test function as it is insensitive to any external physical acceleration. Refer to AN5311 for more details on self-test. Noise density and RMS integrated noise Noise density is defined as the noise per unit of square root bandwidth and is typically expressed in units of mg/√Hz or μg/√Hz for a consumer grade accelerometer. Noise is measured with the device held stationary in a 1g field and isolated from environmental noise and mechanical vibration. The RMS noise at a given ODR can be estimated as follows: Nrms = ND * √BW For example, in the ±2 g FSR, operating in HPM with an ODR of 400 Hz, the estimated RMS noise would be: Nrms = 280 µg/√Hz * √(400/2) Hz = 3.96 mg (~ 4 LSB). Cross-axis sensitivity Cross-axis sensitivity is the ratio of the measured acceleration for an axis to the input acceleration along each axis orthogonal to the measured axis. Cross-axis sensitivity leads to undesirable nonorthogonality of X, Y and Z axes in the frame of reference of the assembled device when mapping to other frames of reference. Cross-axis sensitivity is expressed as a percentage of the orthogonal input acceleration with six separate |
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