MEMS Accelerometers: Testing and Practical Approach For Smart Sensing and Machinery Diagnostics
MEMS Accelerometers: Testing and Practical Approach For Smart Sensing and Machinery Diagnostics
MEMS Accelerometers: Testing and Practical Approach For Smart Sensing and Machinery Diagnostics
1 Introduction
its wide use is its capacity to monitor vibrating machines without interrupting
normal operations. In addition, the vibrating mechanisms of most machineries and
structures are fundamentally well known, giving rise to the possibility of detecting
many faults in accordance with the characteristics of the vibration responses.
Furthermore, the progress of vibration signal processing techniques, computing
capabilities, reliable performance of vibration instrumentation such as wide-band
transducers and portable analysers has caused this technique to be extensively used
around the world.
As an example, in machinery-condition monitoring, accelerometers are often
used to measure their vibration (acceleration) signals, which may lead to the detec-
tion of any deviation from normal signatures. Vibration waveforms are interpreted
and processed in a variety of ways such as peak values and variance of the signal in
the time domain, and power spectral analysis in the frequency domain [4].
Vibration has traditionally been sensed using piezoelectric accelerometers. These
are accurate and reliable, but have some inherent problems: they are difficult
to mass-produce, and they have high source impedance, which means that their
signals must be very carefully amplified. Moreover, the use of the traditional
piezoelectric accelerometers for simultaneous multiple data collection points was
considered to be impractical; this is mainly because of their cost as well as the
costs of the associated electronic signal conditioning units. Other types such as
piezoresistive accelerometers have limited resolution and can be used only for low
and medium frequencies. Low resolution is also a disadvantage of electrodynamic
accelerometers. The capacitive type accelerometers have low resolution and are
fragile. Commercially, several types of accelerometers manufactured by many well-
known manufacturers are available all over the world. In vibration-measurement
filed tests, accelerometers of mainly Integrated Circuit Piezoelectric (ICP) type, are
found not to be able to measure the non-stationary impulsive responses of structures
accurately all the time. However, confidence in measuring impulsive signals using
the charge-type piezoelectric accelerometers is very good [4, 5].
Obviously, the quality of the vibration-based diagnosis and/or identification
of vibration-related problems mainly depends on the measured responses using
accelerometers. Therefore, good performance and high reliability of the com-
mercially available accelerometers is very important. Additionally, the use of
conventional accelerometers for multiple data collection points may increase the
complexity of monitoring system because of the associated electronic units that are
externally connected to the accelerometers. Consequently, the need for cheaper and
more reliable devices is well recognised.
With increasing demands for wireless sensing nodes used for assets control and
condition monitoring; the need for alternatives to those expensive conventional
accelerometers in vibration measurements has risen. Micro-Electro Mechanical
Systems (MEMS) accelerometers are one of the available options because of their
small size, newer technology and low cost, e.g. MEMS accelerometer may be
within 10 % of the cheapest commercially available conventional accelerometers
that come with a signal conditioning unit [4, 5]. According to Yole’s Development
report, the total market for MEMS is expected to exceed $20 Billion in 2020.
2 MEMS Accelerometers: Testing and Practical Approach for Smart Sensing. . . 21
The average price of MEMS accelerometers across all applications decreases, from
an average of $2.50 in 2004 to less than $1.70 in 2015, with consumer applications
driving the price down [6]. MEMS technology is used in some sectors such as
automotive industry for measuring pressure, temperature and air bags systems.
A few earlier researches compared the performance of MEMS accelerometers with
the conventional ones. The main differences are mainly in actuation frequencies,
amplitudes and phase shifts. In general, the selection of accelerometers is based on
their technical specifications and the measurement requirements. The main technical
specifications that decide the use of accelerometers are as the following:
(a) Sensitivity is the ratio of the electrical output of the accelerometer to its
mechanical input. The output usually is expressed in terms of voltage per
unit acceleration. The specification of sensitivity is sufficient for instruments,
which generate their own voltage, independent of an external power source. The
sensitivity of an instrument requiring an external voltage usually is specified in
terms of output voltage per unit of voltage supplied to the instrument per unit
displacement, velocity, or acceleration, e.g. milli-Volts per g of acceleration.
(b) Frequency range is the operating frequency range over which the sensitivity
of the transducer does not vary more than a stated percentage from the
rated sensitivity. The range may be limited by the electrical or mechanical
characteristics of the transducer or by its associated auxiliary equipment.
(c) Amplitude limit specifies the maximum range of acceleration that can be
measured by the accelerometer.
(d) Shock limit represents the maximum level of acceleration the accelerometer can
withstand without any damage to the unit.
(e) Linearity indicates the accuracy of the measured acceleration amplitude within
the corresponding frequency range.
(f) Natural frequency which is indirectly indicative of the measuring frequency
range. In general, a higher natural frequency allows a larger measuring fre-
quency range of an accelerometer.
However, the use of vibration analysis in condition-monitoring is based on three
key points:
1. A frequency component identifies the basic problem.
2. The amplitudes of this component and its harmonics indicate the severity of the
problem.
3. Phase relationships are used to distinguish between looseness and eccentricity
(fault diagnosis).
While a vibration spectrum can reveal much about the ranges of motion and
flexibility (resonance) of a machine, the frequency domain does not yield all the
answers. The time domain is the only place we can identify peak and peak-to-
peak amplitudes of each cycle, phase relationship between signals, and the presence
of such distinctive characteristics as truncated waveforms, pulses and modulation.
The calibration procedure adopted, generally uses the sinusoidal vibration generator
(shaker) with varying frequencies and amplitudes to characterise the accelerometer
22 A. Albarbar and S.H. Teay
A’
A’
a b
Frame
Proof mass
Proof mass
Frame
Beam
Beam
Frame
A
A
Fig. 2.1 Schematic diagram of piezoresistive MEMS accelerometer (a) top view, (b) cross-
sectional view [7]
in each piezoresistor. The corresponding changes are outlined in Table 2.1. One
additional rationale of using Wheatstone bridge is to nullify the defects caused by
temperature drifts in piezoresistors [7, 8].
For packaging design, the piezoresistive MEMS accelerometer is wafer encapsu-
lated with etched glass caps, preventing over-range protection and fluidic squeezed-
film damping. To ensure better measurement experience, the transfer function
between sensor surface and glass gap can be evaluated using their damping
coefficients based on mass-spring-damper mechanical system analysis [8].
Silicon design of capacitive MEMS accelerometer allows low cost mass production
due to the mature technology on surface micromachining. ADXL series from
Analog Devices is one of dominant capacitive MEMS accelerometers in the market
[4]. Application of capacitive MEMS accelerometer include smartphone devices,
smart sensor system and low cost embedded monitoring system. Essentially, the
schematic diagram of capacitive MEMS accelerometer is illustrated in Fig. 2.3.
The movement of the proof mass due to an acceleration of the device changes
the capacitance value between electrodes on stationary fingers. This difference in
24 A. Albarbar and S.H. Teay
a b
Fig. 2.2 Structural schematic of three axis piezoresistive MEMS accelerometer [9] (a) model
view, (b) top and cross-sectional view, (c) equivalent Wheatstone bridge model
Stationary fingers
Anchor to
substrate
Spring
legs
Proof
mass
Inertia force
Fig. 2.3 Schematic diagram breakdown respective circuit model of capacitive MEMS accelerom-
eter [10]
Differential capacitor
Filter
Signal Output
source
Amplifier Synchronous
demodulator
Inverter Feedback
amplifier
Fig. 2.4 Equivalent circuit of the integrated MEMS accelerometer [11, 12]
full-scale range, structural geometry and threshold acceleration [15]. Due to the
complexity of the mechanism, the performance of capacitive MEMS accelerometer
is still far from trivial. Various techniques have been carried to study the variables
of capacitive MEMS accelerometer to optimise its performance and robustness
[16, 17].
2 MEMS Accelerometers: Testing and Practical Approach for Smart Sensing. . . 27
S.
NI DAQ Card
Shaker
Signal
Power amplifier
generator
a 30 MEMS(A)/PCB Accelerometer
FRF Amplitude
20
10
0
−10
−20
0 100 200 300 400 500 600 700 800 900 1000
Frequency(Hz)
30 MEMS(B)/PCB Accelerometer
FRF Amplitude
20
10
0
−10
−20
0 100 200 300 400 500 600 700 800 900 1000
Frequency(Hz)
30 MEMS(C)/PCB Accelerometer
FRF Amplitude
20
10
−10
−20
0 100 200 300 400 500 600 700 800 900 1000
Frequency(Hz)
b 500
MEMS(A)/PCB Accelerometer
FRF Phase(deg)
−500
100 200 300 400 500 600 700 800 900 1000
Frequency(Hz)
500
MEMS(B)/PCB Accelerometer
FRF Phase(deg)
−500
100 200 300 400 500 600 700 800 900 1000
Frequency(Hz)
500
MEMS(C)/PCB Accelerometer
FRF Phase(deg)
−500
100 200 300 400 500 600 700 800 900 1000
Frequency(Hz)
Fig. 2.6 MEMS accelerometer’s response (a) magnitude and (b) phase of the frequency [4]
30 A. Albarbar and S.H. Teay
4 Packaging Technique
In this section, MEMS accelerometers are used to collect vibration data from two
types of rotating machinery: a DC motor and a CNC machine. These two types of
machines are widely used in today’s industry, and it would be of great importance
2 MEMS Accelerometers: Testing and Practical Approach for Smart Sensing. . . 31
a 5 b 1
4.5 0.9
4 0.8
3 0.6
2.5 0.5
2 0.4
1.5 0.3
1 0.2
0.5 0.1
0 0
0 0.05 0.1 0.15 0.2 0.25 0.3 0.35 0.4 0 50 100 150 200 250
Time (sec) Frequency (Hz)
5 1
c d
4.5 0.9
4 0.8
3.5 Amplitude (arbitrary units) 0.7
Voltage (V)
3 0.6
2.5 0.5
2 0.4
1.5 0.3
1 0.2
0.5 0.1
0 0
0 0.05 0.1 0.15 0.2 0.25 0.3 0.35 0.4 0 50 100 150 200 250
Time (sec) Frequency (Hz)
Fig. 2.8 Calibrated vibration waveform of ADXL001-70: (a) 0 Hz, 0 ms2 , (b) frequency domain,
(c) 79.6 Hz, 10 ms2 , (d) frequency domain
The DC motor test rig is shown in Fig. 2.13. It consists of a DC motor attached to a
shaft supported by three roller bearing and holds a metallic disk. The motor’s speed
is controlled by a speed controller, which varies from 0 rpm to a maximum rotational
speed of 2864 rpm. An ADXL001-70 MEMS accelerometer, placed on drive end
bearing housing, is used to collect the vibration data at five different speeds: 280,
914, 1602, 2281 and 2864 rpm. Time and frequency domains of collected vibration
data are shown in Fig. 2.14. The respective harmonics could be seen, in particular,
at rotational speeds higher than 1602 rpm.
32 A. Albarbar and S.H. Teay
1
ADXL-001-70
0.9 Conventional accelerometer
0.8
0.7
Normalised PSD
0.6
0.5
0.4
0.3
0.2
0.1
0
0 50 100 150 200 250 300 350 400
Frequency (Hz)
Fig. 2.9 Frequency spectrum of acquired vibration signal using ADXL001-70 and conventional
accelerometer at 50 Hz
0.9
0.8
0.7
0.6
Coherence
0.5
0.4
0.3
0.2
0.1
0
0 50 100 150 200 250 300 350 400
Frequency (Hz)
Fig. 2.10 Coherence between the vibration signals acquired using ADXL001-70 and conventional
accelerometer
2 MEMS Accelerometers: Testing and Practical Approach for Smart Sensing. . . 33
+5v
0v
1nF 1nF
8 5
0.1µF VDD XOUT
AADXL202AE
3 6
COM YFILT
2 7
1MΩ T2 XFILT
4 2
YOUT ST
Fig. 2.12 MEMS packaged sensor components: (a) sensor outer casing (mild steel), (b) threaded
mounting bottom plate, (c) flat mounting bottom plate with MEMS affixed, (d) MEMS with
components attached, (e) Packaged MEMS sensor
a
2 4.88Hz
Voltage (V)
|Y(f)|
0
0 10
−2
|Y(f)|
0
0 10
−2
2
Voltage (V)
|Y(f)|
0
0 10
−2
2
Voltage (V)
|Y(f)|
0
0 10
−2
2
Voltage (V)
|Y(f)|
0
0 10
−2
Fig. 2.14 DC motor vibration and power spectrum measured by ADXL001-70 at different rotating
speeds: (a) 280 rpm (4.67 Hz), (b) 914 rpm (15.23 Hz), (c) 1602 rpm (26.7 Hz), (d) 2281 rpm (38
Hz), (e) 2864 rpm (47.73 Hz)
a b
Fig. 2.16 CNC machine vibration measured by ADXL001-7 at speed of 2400 rpm (a) time
domain and (b) frequency domain [4]
The CNC machine was run at 2400 rpm, and at this speed the fundamental speed
and harmonics are 40, 80 and 160 Hz which were clearly presented in the frequency
domain of Fig. 2.16.
Power supply
a b Passive electronic
components incl.
transistor bank
Data
storage
module
Wireless
communication
Sensing device
channel
Fig. 2.18 Working prototype of MEMS-based smart sensor system (a) prospective view and
(b) top layout view
Start
Signal conditioning in
peripheral
computational unit
Signal processing in
main computational
unit
Data classification
Turn sensor to
hibernate mode
7 Concluding Remarks
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