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FXLS8964AF 数据表(PDF) 9 Page - NXP Semiconductors

部件名 FXLS8964AF
功能描述  3-Axis Low-g Accelerometer
PDF  98 Pages
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制造商  NXP [NXP Semiconductors]
网页  http://www.nxp.com
标志 NXP - NXP Semiconductors

FXLS8964AF 数据表(HTML) 9 Page - NXP Semiconductors

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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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