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ADIS16006/PCB 数据表(PDF) 13 Page - Analog Devices

部件名 ADIS16006/PCB
功能描述  Dual-Axis -5 Accelerometer with SPI Interface
PDF  16 Pages
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制造商  AD [Analog Devices]
网页  http://www.analog.com
标志 AD - Analog Devices

ADIS16006/PCB 数据表(HTML) 13 Page - Analog Devices

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ADIS16006
Rev. 0 | Page 13 of 16
SETTING THE BANDWIDTH
The ADIS16006 has provisions for band limiting the acceler-
ometer. Capacitors can be added at the XFILT and YFILT pins
to implement further low-pass filtering for antialiasing and
noise reduction. The equation for the 3 dB bandwidth is
F−3dB = 1/(2π(32 kΩ) × (C(XFILT, YFILT) + 2200 pF))
or more simply,
F−3dB = 5 μF/(C(XFILT, YFILT) + 2200 pF)
The tolerance of the internal resistor (RFILT) can vary typically as
much as ±25% of its nominal value (32 kΩ); thus, the bandwidth
varies accordingly.
A minimum capacitance of 0 pF for CXFILT and CYFILT is
allowable.
Table 9. Filter Capacitor Selection, CXFILT and CYFILT
Bandwidth (Hz)
Capacitor (μF)
1
4.7
10
0.47
50
0.10
100
0.047
200
0.022
400
0.01
2250
0
SELECTING FILTER CHARACTERISTICS:
THE NOISE/BANDWIDTH TRADE-OFF
The accelerometer bandwidth selected ultimately determines
the measurement resolution (smallest detectable acceleration).
Filtering can be used to lower the noise floor, which improves
the resolution of the accelerometer. Resolution is dependent on
the analog filter bandwidth at XFILT and YFILT.
The ADIS16006 has a typical bandwidth of 2.25 kHz with no
external filtering. The analog bandwidth may be further
decreased to reduce noise and improve resolution.
The ADIS16006 noise has the characteristics of white Gaussian
noise, which contributes equally at all frequencies and is described
in terms of μg/√Hz (that is, the noise is proportional to the
square root of the accelerometer’s bandwidth). The user should
limit bandwidth to the lowest frequency needed by the applica-
tion to maximize the resolution and dynamic range of the
accelerometer.
With the single pole roll-off characteristic, the typical noise of
the ADIS16006 is determined by
rmsNoise = (200 μg/root Hz) x (root (BW x 1.57))
At 100 Hz, the noise is
rmsNoise = (200 μg/root Hz) x (root (100 x 1.57)) =2.5 mg
Often, the peak value of the noise is desired. Peak-to-peak noise
can be estimated only by statistical methods. Table 10 is useful
for estimating the probabilities of exceeding various peak
values, given the rms value.
Table 10. Estimation of Peak-to-Peak Noise
Peak-to-Peak
Value
Percentage of Time That Noise Exceeds
Nominal Peak-to-Peak Value
2 × rms
32%
4 × rms
4.6%
6 × rms
0.27%
8 × rms
0.006%
12
4
10
11
6
5
8
9
7
3
2
1
8
9
7
3
2
1
12
4
10
11
6
5
Top View
Not to Scale
DIGITAL OUTPUT (IN LSBs)
X-AXIS: 1792
Y-AXIS: 2048
DIGITAL OUTPUT (IN LSBs)
X-AXIS: 2304
Y-AXIS: 2048
DIGITAL OUTPUT (IN LSBs)
X-AXIS: 2048
Y-AXIS: 2304
DIGITAL OUTPUT (IN LSBs)
X-AXIS: 2048
Y-AXIS: 1792
DIGITAL OUTPUT (IN LSBs)
X-AXIS: 2048
Y-AXIS: 2048
Figure 23. Output Response vs. Orientation



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