3.1. Assessment of the Low-Cost Sensing Node
In this section, results of experimental surveys performed to validate the developed sensing node are reported. For the sake of convenience, it must be considered that the device resolution has already been investigated in [
16], leading to the results shown in
Table 2.
In order to test the system response to acceleration stimuli, the experimental setup shown in
Figure 9a is used, equipped with the APS 129 HF ELECTRO-SEIS
® long-stroke vibration exciter, available at the Experimental Dynamics Laboratory of the L.E.D.A. Research Institute at the University of Enna “Kore”, Enna, Italy [
22]. The sensing platform is fixed to the moving platform of the shaker. The system, after a settling time, performs 10 reliable periods at the desired frequency and amplitude. The reference value is provided by a QA-700 accelerometer by Honeywell, Charlotte, NC, USA, whose main characteristics are as follows:
Operating range: ±30 g;
Bias: <8 mg;
One-year composite repeatability: <1200 μg;
Temperature sensitivity: <70 µg/°C;
Intrinsic noise: <7 µg rms (0–10 Hz), 70 µg rms (10–500 Hz).
Characteristics of stimulation signals are reported in
Table 3 in terms of their nominal frequency and amplitude values.
Figure 9b shows the concatenation of 10 periods of the signal recorded by the sensing node for each considered frequency [
17]. Results obtained by the wavelet analysis, shown in
Figure 9c [
17], as well as the discrete Fourier transforms shown in
Figure 9d, confirm the compliance of the system response to the applied stimulus.
In order to quantify such performances, the following index has been defined:
where
V states for the amplitude,
A, or the frequency,
f, of the applied stimulus.
Moreover, the repeatability, assessing the system performances in the acceleration domain, is estimated as 3 times the standard deviation of peak values distribution. The results obtained for above defined indexes, under different operating conditions, are shown in
Figure 10. The
δA, for the three axes, is limited to under 1% in most of the investigated frequencies, with the exception of a few cases where its value reaches 5%. The
δf values show that the frequency discrepancy is extremely low (less than 0.03%) for each solicitation frequency and for each axis. The repeatability has an upward trend with the frequency, which rises after 10 Hz, being, however, confined below 4.5% of the nominal values.
The next set of experiments is dedicated to testing the system response to dynamics imposed by using a controlled moving platform. The sensing node is hooked at the center of the vibrating platform, as shown in
Figure 11. The vibrating platform has 6 degrees of freedom, with ±1.5 g horizontal acceleration range, ±1 g vertical acceleration range, and an RT3-S real-time digital control system, exploiting a 2 kHz control loop in position, velocity, and acceleration. A detailed description of the shaking table facility is reported in [
23,
24]. For the sake of comparison and validation, a dedicated reference system has been used, which consists of eight MEMS DC accelerometers (model 3711B1110G by PCB Piezotronics, Depew, NY, USA) placed in the actuator of the vibrating platform (two along the
X-axis, two along the
Y-axis, and four along the
Z-axis), whose main specifications are as follows:
In particular, the response of the sensing node to the following signals is observed:
Frequency sweep test: an acceleration stimulus, ranging from 0.5 Hz to 20 Hz, applied along the X, Y, and Z-axes;
Tilt test: a periodic tilt, ranging from −2.5° to 2.5°, applied for two different frequency values;
Seismic test: a typical seismic signal.
The results obtained for the frequency sweep test are reported in
Figure 12, which shows the output from both the reference system and the sensing platform.
Figure 13 shows the wavelet power spectrum of the above signals [
25]. In particular, to achieve this goal, the synchrosqueezing wavelet is used to narrow the frequency distribution in each time instant. The time–frequency analysis clearly demonstrates the coherence with the adopted frequency sweep stimulus.
The following indexes are used in order to assess the performance of the sensing platform:
where
ζ estimates the percentage error with respect to the nominal values on the whole signal;
V1, V2 are signals recorded by the reference system and the sensing node, respectively;
n is the number of samples;
is the cross-correlation between the two signals, V1 and V2, as a function of the lag (l);
Rnorm is the normalized cross-correlation between the reference and the acquired signals, defined in l = 0.
Moreover, the following index,
, representing the normalized cross-correlation in the time–frequency domain, is used to assess the similarity of the time–frequency content of the sensor output against the reference signal:
where
The results obtained for performance indexes (6), (8), and (9) are reported in
Table 4. High values of R_norm (close to 1.0) for the three axes prove the capability of the sensing platform to follow the dynamics of the solicitation in the whole investigated frequency range. Values of C_norm are over 0.9, which demonstrates the coherence in the frequency domain of the two signals. The ζ values provide a quantification of the difference in magnitude between the two signals, which, on average, is about 8.5%. As can be observed, the
Z and
Y axes show higher ζ values with respect to the
X-axis, most probably due to the presence of noise superimposed to the output signal along these directions. Further investigations will be dedicated to identifying possible strategies aimed at reducing the effect of such influencing quantities on the system performance.
Concerning the tilt test, the vibrating platform generates a series of oscillations at fixed frequencies (0.2 Hz and 0.5 Hz) in the range of ±2.5°. The test is performed through the
X and
Y axes (as defined in
Figure 11) of the sensor node, which is intended to measure a quasi-static tilt.
Figure 14 shows the time series provided by both the reference system and the sensing platform. Performance indexes (6), (8), and (9) calculated for this test are reported in
Table 5. As can be observed, estimated values for ζ are lower than 4%, and values of
Rnorm and
Cnorm are close to 1 for both considered axes. Such results demonstrate the capability of the sensor node to follow the imposed solicitation.
During the last test on the accelerometer, the vibrating platform was used to reproduce the ground motion recorded during a real earthquake. Particularly, the tree components of the Kobe earthquake, recorded in Takatori, Japan, on 16 January 1995, were used. This event was characterized by high horizontal and vertical ground motion (
Mw = 6.9). The test aimed to validate the sensing platform response to this kind of realistic complex solicitation (rich magnitude and frequency content).
Figure 15 shows output signals of both the reference system and the sensing platform, for the three axes. From the wavelet analysis, shown in
Figure 16, it is possible to observe that the energy of the wavelet in the
X and
Y axes is mainly located in the low-frequency range, while the response along the
Z-axis shows relevant energy content for higher frequency.
Table 6 reports performance indexes (6), (8), and (9) calculated for this test. Values of
are close to 1.0 for the three axes, thus validating the capability of the node to measure input with rich frequency content. Values obtained for the index ζ, along the
X and
Y axes are in line with the previous test, resulting in values below than 6%. Values of
for the
X and
Y axes confirm a suitable coherence in the time–frequency domain between the sensing node and the reference system, while highlighting lower coherence for the
Z-axis. The worst performances observed for the
Z-axis are most probably due to the presence of high-frequency noise along this direction.