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20 pages, 122916 KiB  
Article
A Reef’s High-Frequency Soundscape and the Effect on Telemetry Efforts: A Biotic and Abiotic Balance
by Frank McQuarrie, C. Brock Woodson and Catherine R. Edwards
J. Mar. Sci. Eng. 2025, 13(3), 517; https://doi.org/10.3390/jmse13030517 - 7 Mar 2025
Viewed by 84
Abstract
Acoustic telemetry is a tool for tracking animals, but transmitted signals from tagged animals are not always detected. Detection efficiency declines with increasing background noise, which can have both abiotic and biotic sources. The abiotic noise present in reef environments (waves, bubbles, etc.) [...] Read more.
Acoustic telemetry is a tool for tracking animals, but transmitted signals from tagged animals are not always detected. Detection efficiency declines with increasing background noise, which can have both abiotic and biotic sources. The abiotic noise present in reef environments (waves, bubbles, etc.) is primarily low-frequency, but snapping shrimp create high-frequency noise that can interfere with transmission detections. Prior work in shallow coastal reefs correlated winds with less high-frequency background noise, and hypothesized that it was due to a balance of biotic and/or abiotic factors: shrimp may be less active during high wind events, and sound attenuation at the surface increases with wave height. To test this hypothesis, passive acoustic recordings from a live-bottom reef are used to quantify snapping shrimp snap rate. Snap rate was strongly correlated with temperature, and warmer environments appeared to be challenging for acoustic telemetry. However, the majority of synoptic variability in noise is shown to be driven by abiotic attenuation. Wind speed has little to no effect on snapping shrimp behavior, but has a significant inverse correlation with high-frequency noise levels due to surface attenuation of high-frequency noise, and therefore a positive effect on detection efficiency, pointing to primarily abiotic forcing behind noise variability and resulting telemetry success. This research gives context to previously collected detection data and can be leveraged to help plan future acoustic arrays in shallow, complex, and/or noisy environments, potentially predicting changes in detection range. Full article
(This article belongs to the Special Issue Recent Advances in Marine Bioacoustics)
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<p>Schematic detailing the hypothesized relationships between wind and detection efficiency. (<b>A</b>) The biotic hypothesis: As winds increase, snapping shrimp are less active. leading to less noise being created and higher detection efficiency of transmissions. (<b>B</b>) The abiotic hypothesis: As winds increase, snapping shrimp are unaffected and create the same amount of noise, but there is significant sound attenuation due to surface bubble loss (SBL). Illustration by Lee Ann DeLeo (SkIO/UGA).</p>
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<p>Habitat characterization for SURTASSTN20 at GRNMS. Colors denote bottom composition. Map credit: Alison Soss (NOAA/GRNMS).</p>
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<p>SoundTrap 500 recordings were bandpass-filtered (1.5–20 kHz), visualized in Raven Pro as (<b>A</b>) full-spectrum waveform with RMS amplitude (blue) and (<b>B</b>) spectrogram, plotting intensity (dB FS/Hz) normalized to 1 Hz bandwidth. (<b>C</b>) Example waveform amplitude (blue line) identifying single snap exceeding 1000 U threshold (shaded in red); (<b>D</b>) spectrogram from same time (snap shaded in red).</p>
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<p>Surface Bubble Loss (SBL) calculated at 69 kHz, the transmission frequency and center of the HF noise measurement (50–90 kHz). A range of angles from 2 to 90° are plotted with 10° bolded to highlight the angle chosen for this analysis. Lower angles and higher frequencies increase SBL attenuation.</p>
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<p>Temporal variability at SURTASSTN20. (<b>A</b>) Low-pass-filtered bottom temperature (light green, dashed) and snapping shrimp snap rate (dark green, solid) in (<b>A</b>) spring and (<b>B</b>) fall. (<b>C</b>) Snap rate (green) is plotted with night time shaded to highlight crepuscular and diurnal behavior patterns. Times in UTC.</p>
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<p>Canonical day averages: HF noise (gray), shrimp snap rate (green), and hourly detections (red). HF noise and transmission detections are from SURTASS05IN.</p>
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<p>Binned averaging from the Spring deployment at SURTASSTN20. (<b>A</b>) Low-frequency (0.17–0.36 kHz) noise measured by SoundTrap 500 hydrophone; (<b>B</b>) high-frequency (50–90 kHz) noise measured by VR2Tx transceiver, and detection efficiency between SURTASSTN20 and STSNew1. The formation of whitecaps is noted vertically (–).</p>
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<p>Comparison between (<b>A</b>,<b>B</b>) calm and (<b>C</b>,<b>D</b>) high-wind scenarios. Low-frequency (0.17–0.36 kHz) noise was measured by SoundTrap 500 hydrophone; high-frequency (50–90 kHz) noise was measured by VR2Tx transceiver. Nighttime is shaded.</p>
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<p>Data from SURTASSTN20 in Spring 2020. Calculated SBL (blue dashed) versus (<b>A</b>) snapping shrimp activity (green), (<b>B</b>) HF noise (black), and (<b>C</b>) detection efficiency (red) between SURTASSTN20 and STSNew1, 440 m away.</p>
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<p>Hourly averages from spring (n = 2268 h) of (<b>A</b>) raw and (<b>B</b>) filtered snap rate and HF noise (mV), on log scale; (<b>C</b>) raw and (<b>D</b>) filtered SBL (dB) and HF noise (mV); (<b>E</b>) raw and (<b>F</b>) filtered snap rate and wind speed (m/s). Marker color represents date range, January (blue) to May (yellow). Reported statistics include all plotted data; “no significance” represents <span class="html-italic">p</span>-values &gt; 0.01. Binned averages are shown over raw data (black markers) in (<b>A</b>,<b>C</b>,<b>E</b>), and significant wind events are denoted (black lines) in (<b>B</b>,<b>D</b>,<b>F</b>). See <a href="#jmse-13-00517-f011" class="html-fig">Figure 11</a> for closer examination of isolated wind event (*).</p>
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<p>Example of a single wind event, 19–25 February 2020, with 0.3–14.3 m/s wind speed. (<b>A</b>) Raw and (<b>B</b>) low-pass SBL (dB) and HF noise (mV), (<b>C</b>) raw and (<b>D</b>) low-pass SBL (dB) and detections, and (<b>E</b>) raw and (<b>F</b>) low-pass SBL (dB) and snap rate.</p>
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<p>Data from SURTASSTN20, 22 April to 4 May 2020. (<b>A</b>) Glider data measuring the water column’s bulk density stratification (color); (<b>B</b>) HF noise (black) plotted against hourly detections (red) between SURTASSTN20 and STSNew1, with “challenging environment” (650 mV) denoted (–); (<b>C</b>) calculated SBL (blue) and AUV-measured density stratification (black); (<b>D</b>) snap rate binned hourly (green). All times in UTC.</p>
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15 pages, 2246 KiB  
Article
Cost-Effective Photoacoustic Imaging Using High-Power Light-Emitting Diodes Driven by an Avalanche Oscillator
by Alberto Prud’homme and Frederic Nabki
Sensors 2025, 25(6), 1643; https://doi.org/10.3390/s25061643 - 7 Mar 2025
Viewed by 139
Abstract
Photoacoustic imaging (PAI) is an emerging modality that merges optical and ultrasound imaging to provide high-resolution and functional insights into biological tissues. This technique leverages the photoacoustic effect, where tissue absorbs pulsed laser light, generating acoustic waves that are captured to reconstruct images. [...] Read more.
Photoacoustic imaging (PAI) is an emerging modality that merges optical and ultrasound imaging to provide high-resolution and functional insights into biological tissues. This technique leverages the photoacoustic effect, where tissue absorbs pulsed laser light, generating acoustic waves that are captured to reconstruct images. While lasers have traditionally been the light source for PAI, their high cost and complexity drive interest towards alternative sources like light-emitting diodes (LEDs). This study evaluates the feasibility of using an avalanche oscillator to drive high-power LEDs in a basic photoacoustic imaging system. An avalanche oscillator, utilizing semiconductor avalanche breakdown to produce high-voltage pulses, powers LEDs to generate short, high-intensity light pulses. The system incorporates an LED array, an ultrasonic transducer, and an amplifier for signal detection. Key findings include the successful generation of short light pulses with sufficient intensity to excite materials and the system’s capability to produce detectable photoacoustic signals in both air and water environments. While LEDs demonstrate cost-effectiveness and portability advantages, challenges such as lower power and broader spectral bandwidth compared to lasers are noted. The results affirm that LED-based photoacoustic systems, though currently less advanced than laser-based systems, present a promising direction for affordable and portable imaging technologies. Full article
(This article belongs to the Special Issue Photonics for Advanced Spectroscopy and Sensing)
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<p>Diagram of the avalanche oscillator with LED array.</p>
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<p>Schematic of the amplification circuit.</p>
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<p>(<b>a</b>) Light pulse duration measurement setup without temporal blockage; (<b>b</b>) light pulse duration measurement setup with blockage.</p>
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<p>Experimental setup showing the LED, microphone, and black polyethylene membrane in a 3D-printed PETG casing for photoacoustic signal detection in air.</p>
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<p>Experimental setup for system characterization in distilled water, showing the LED, transducer, and chlorophyll sample in a Pyrex recipient.</p>
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<p>Oscillator output pulse measurements: (<b>a</b>) without LED connected, using a 50-ohm resistor; (<b>b</b>) with LED connected to the oscillator output.</p>
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<p>Comparison of electrical and optical pulse measurements. Electrical pulse supplied to the LED (red) and corresponding light pulse measured by the TIA (green). (<b>a</b>) Pulse duration measurement without blockage, and (<b>b</b>) pulse duration measurement with blockage.</p>
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<p>Acoustic signal evaluation: (<b>a</b>) TIA output without a membrane, showing no acoustic response (green) from the electrical excitation signal from the oscillator (red); (<b>b</b>) TIA output with a membrane, showing a detectable acoustic response (green) following the electrical excitation pulse (red).</p>
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<p>(<b>a</b>) Photoacoustic signal measured in water; (<b>b</b>) zoomed-in view of the photoacoustic signal measured in water.</p>
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28 pages, 18090 KiB  
Article
AFSA-FastICA-CEEMD Rolling Bearing Fault Diagnosis Method Based on Acoustic Signals
by Jin Yan, Fubing Zhou, Xu Zhu and Dapeng Zhang
Mathematics 2025, 13(5), 884; https://doi.org/10.3390/math13050884 (registering DOI) - 6 Mar 2025
Viewed by 149
Abstract
As one of the key components in rotating machinery, rolling bearings have a crucial impact on the safety and efficiency of production. Acoustic signal is a commonly used method in the field of mechanical fault diagnosis, but an overlapping phenomenon occurs very easily, [...] Read more.
As one of the key components in rotating machinery, rolling bearings have a crucial impact on the safety and efficiency of production. Acoustic signal is a commonly used method in the field of mechanical fault diagnosis, but an overlapping phenomenon occurs very easily, which affects the diagnostic accuracy. Therefore, effective blind source separation and noise reduction of the acoustic signals generated between different devices is the key to bearing fault diagnosis using acoustic signals. To this end, this paper proposes a blind source separation method based on an AFSA-FastICA (Artificial Fish Swarm Algorithm, AFSA). Firstly, the foraging and clustering characteristics of the AFSA algorithm are utilized to perform global optimization on the aliasing matrix W, and then inverse transformation is performed on the global optimal solution W, to obtain a preliminary estimate of the source signal. Secondly, the estimated source signal is subjected to CEEMD noise reduction, and after obtaining the modal components of each order, the number of interrelationships is used as a constraint on the modal components, and signal reconstruction is performed. Finally, the signal is subjected to frequency domain feature extraction and bearing fault diagnosis. The experimental results indicate that, the new method successfully captures three fault characteristic frequencies (1fi, 2fi, and 3fi), with their energy distribution concentrated in the range of 78.9 Hz to 228.7 Hz, indicative of inner race faults. Similarly, when comparing the different results with each other, the denoised source signal spectrum successfully captures the frequencies 1fo, 2fo, and 3fo and their sideband components, which are characteristic of outer race faults. The sideband components generated in the above spectra are preliminarily judged to be caused by impacts between the fault location and nearby components, resulting in modulated frequency bands where the modulation frequency corresponds to the rotational frequency and its harmonics. Experiments show that the method can effectively diagnose the bearing faults. Full article
(This article belongs to the Special Issue Numerical Analysis in Computational Mathematics)
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<p>Artificial Fish Swarm Algorithm Model: (<b>a</b>) Continuous Vision Model, (<b>b</b>) Discrete Vision Model.</p>
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<p>FastICA Algorithm Process.</p>
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<p>CEEMD Flowchart.</p>
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<p>ASFA-FastICA-CEEMD.</p>
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<p>Source Signals.</p>
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<p>Mixed Signals.</p>
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<p>Acoustic Separation Signals Based on the Artificial Fish Swarm Algorithm.</p>
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<p>Continuation of Acoustic Separation Signals Based on the Artificial Fish Swarm Algorithm.</p>
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<p>Continuation of Acoustic Separation Signals Based on the Artificial Fish Swarm Algorithm.</p>
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<p>FastICA Acoustic Separation Signals.</p>
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<p>FastICA Acoustic Separation Signals.</p>
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<p>Continuation of FastICA Acoustic Separation Signals.</p>
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<p>Artificial Fish Swarm Algorithm vs. Original FastICA Algorithm.</p>
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<p>Time-Domain Waveform of Simulated Signal and Decomposed Signals. (<b>a</b>) Time-domain waveform of the simulated signal, (<b>b</b>) CEEMD decomposed signal, (<b>c</b>) EMD decomposed signal, (<b>d</b>) EEMD decomposed signal.</p>
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<p>Bearing Fault Test Platform.</p>
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<p>Acoustic Signal Sensor Array.</p>
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<p>Without Acoustic Signal Separation: (<b>a</b>) Rolling element fault, (<b>b</b>) Cage fault, (<b>c</b>) Inner race fault, (<b>d</b>) Outer race fault.</p>
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<p>Without Acoustic Signal Separation: (<b>a</b>) Rolling element fault, (<b>b</b>) Cage fault, (<b>c</b>) Inner race fault, (<b>d</b>) Outer race fault.</p>
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<p>Time-domain Waveform After Separation: (<b>a</b>) Rolling element fault, (<b>b</b>) Cage fault, (<b>c</b>) Inner race fault, (<b>d</b>) Outer race fault.</p>
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<p>Spectral Features After Acoustic Signal Separation: (<b>a</b>) Rolling element fault, (<b>b</b>) Cage fault, (<b>c</b>) Inner race fault, (<b>d</b>) Outer race fault.</p>
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<p>IMF Components: (<b>a</b>) Rolling element fault, (<b>b</b>) Cage fault, (<b>c</b>) Inner race fault, (<b>d</b>) Outer race fault.</p>
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<p>Time-domain Waveform After Denoising: (<b>a</b>) Rolling element fault, (<b>b</b>) Cage fault, (<b>c</b>) Inner race fault, (<b>d</b>) Outer race fault.</p>
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<p>Spectral Features After CEEMD Denoising: (<b>a</b>) Rolling element fault, (<b>b</b>) Cage fault, (<b>c</b>) Inner race fault, (<b>d</b>) Outer race fault.</p>
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<p>Spectral Features After CEEMD Denoising: (<b>a</b>) Rolling element fault, (<b>b</b>) Cage fault, (<b>c</b>) Inner race fault, (<b>d</b>) Outer race fault.</p>
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23 pages, 7767 KiB  
Article
Novel Real-Time Acoustic Power Estimation for Dynamic Thermoacoustic Control
by Eduardo Pilo de la Fuente, Jaime Gros, María Antonia Simón Rodríguez, Ana-Isabel Velasco and Carmen Iniesta
Appl. Sci. 2025, 15(5), 2838; https://doi.org/10.3390/app15052838 - 6 Mar 2025
Viewed by 109
Abstract
This paper presents a new procedure for the real-time processing and analysis of data from thermoacoustic systems. The approach focuses on continuously acquiring and adjusting measurements of acoustic wave pressure, enabling the instantaneous estimation of acoustic power. This is crucial for real-time control [...] Read more.
This paper presents a new procedure for the real-time processing and analysis of data from thermoacoustic systems. The approach focuses on continuously acquiring and adjusting measurements of acoustic wave pressure, enabling the instantaneous estimation of acoustic power. This is crucial for real-time control and decision-making, especially in applications that require rapid power estimation, such as the control loop implementation in thermoacoustic engines, where conditions are constantly changing and dynamic adaptation is essential. Two methods for estimating the power delivered to the load are proposed: (method 1) instantaneous power evaluation, which calculates the power consumed by the resistance in the resistance–capacitance (RC) load, and (method 2) one-period average power calculation using the well-established two-microphones method. These methods are validated with both different synthetic signals and experimental measurements. The results reveal that the new method provides real-time accurate estimations of the power delivered to the acoustic load and, thus, has shown potential for control-based applications. Full article
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<p>Illustration of the acoustic power visualization through a low-cost display.</p>
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<p>Diagram of a thermoacoustic resistance–capacitance (RC) load. <math display="inline"><semantics> <mrow> <msub> <mi>P</mi> <mi>C</mi> </msub> </mrow> </semantics></math>, <math display="inline"><semantics> <mrow> <msub> <mi>P</mi> <mi>E</mi> </msub> </mrow> </semantics></math>, and <math display="inline"><semantics> <mrow> <msub> <mi>P</mi> <mi>V</mi> </msub> </mrow> </semantics></math> are the pressures at the compliance, the resonator, and the valve, respectively. <math display="inline"><semantics> <mi>U</mi> </semantics></math> is the volume flow rate through the valve.</p>
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<p>Electric RC load, where V<sub>C</sub>, V<sub>g</sub>, and V<sub>R</sub> are the voltages at the capacitor, the source, and the resistor and I is the current though the circuit.</p>
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<p>Phasor diagram of an RC load.</p>
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<p>Voltage, current, and instantaneous power in a resistive element.</p>
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<p>Estimation of the average value of the signal based on the previous cycle.</p>
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<p>Estimation of the average value of the signal based on the first cycle.</p>
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<p>Moving-average-based filtering of the drawing, with W = 3.</p>
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<p>Identification of relevant quantities of the signal for method.</p>
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<p>Estimation of the direct current (DC) component of the signal of <math display="inline"><semantics> <mrow> <msub> <mi>P</mi> <mi>E</mi> </msub> <mfenced> <mi>k</mi> </mfenced> </mrow> </semantics></math> and <math display="inline"><semantics> <mrow> <msub> <mi>P</mi> <mi>C</mi> </msub> <mfenced> <mi>k</mi> </mfenced> </mrow> </semantics></math> (ideal signals).</p>
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<p>Alternating current (AC) component of <math display="inline"><semantics> <mrow> <msub> <mi>P</mi> <mi>E</mi> </msub> <mfenced> <mi>k</mi> </mfenced> </mrow> </semantics></math> and <math display="inline"><semantics> <mrow> <msub> <mi>P</mi> <mi>C</mi> </msub> <mfenced> <mi>k</mi> </mfenced> </mrow> </semantics></math> analyzed for ideal signals, considering both non-filtered and filtered cases.</p>
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<p>Instantaneous power obtained using Equation (22) for ideal signals.</p>
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<p>AC component of <math display="inline"><semantics> <mrow> <msub> <mi>P</mi> <mi>E</mi> </msub> <mfenced> <mi>k</mi> </mfenced> </mrow> </semantics></math> and <math display="inline"><semantics> <mrow> <msub> <mi>P</mi> <mi>C</mi> </msub> <mfenced> <mi>k</mi> </mfenced> </mrow> </semantics></math>, filtered and non-filtered, with different noise levels (uniformly distributed noise).</p>
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<p>AC component of <math display="inline"><semantics> <mrow> <msub> <mi>P</mi> <mi>E</mi> </msub> <mfenced> <mi>k</mi> </mfenced> </mrow> </semantics></math> and <math display="inline"><semantics> <mrow> <msub> <mi>P</mi> <mi>C</mi> </msub> <mfenced> <mi>k</mi> </mfenced> </mrow> </semantics></math>, filtered and non-filtered, with different noise levels (gaussian noise).</p>
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<p>AC component of <math display="inline"><semantics> <mrow> <msub> <mi>P</mi> <mi>E</mi> </msub> <mfenced> <mi>k</mi> </mfenced> </mrow> </semantics></math> and <math display="inline"><semantics> <mrow> <msub> <mi>P</mi> <mi>C</mi> </msub> <mfenced> <mi>k</mi> </mfenced> </mrow> </semantics></math>, filtered and non-filtered, with different noise levels (harmonic noise, 400 Hz).</p>
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<p>AC component of <math display="inline"><semantics> <mrow> <msub> <mi>P</mi> <mi>E</mi> </msub> <mfenced> <mi>k</mi> </mfenced> </mrow> </semantics></math> and <math display="inline"><semantics> <mrow> <msub> <mi>P</mi> <mi>C</mi> </msub> <mfenced> <mi>k</mi> </mfenced> </mrow> </semantics></math>, filtered and non-filtered, with different sampling periods.</p>
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<p>Experimental values of <math display="inline"><semantics> <mrow> <msub> <mi>P</mi> <mi>E</mi> </msub> <mfenced> <mi>k</mi> </mfenced> </mrow> </semantics></math> and <math display="inline"><semantics> <mrow> <msub> <mi>P</mi> <mi>C</mi> </msub> <mfenced> <mi>k</mi> </mfenced> </mrow> </semantics></math> for measured signals, showing amplitude variations (red line).</p>
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<p>Estimation of the DC component of the signal of <math display="inline"><semantics> <mrow> <msub> <mi>P</mi> <mi>E</mi> </msub> <mfenced> <mi>k</mi> </mfenced> </mrow> </semantics></math> and <math display="inline"><semantics> <mrow> <msub> <mi>P</mi> <mi>C</mi> </msub> <mfenced> <mi>k</mi> </mfenced> </mrow> </semantics></math> for measured signals.</p>
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<p>AC component of <math display="inline"><semantics> <mrow> <msub> <mi>P</mi> <mi>E</mi> </msub> <mfenced> <mi>k</mi> </mfenced> </mrow> </semantics></math> and <math display="inline"><semantics> <mrow> <msub> <mi>P</mi> <mi>C</mi> </msub> <mfenced> <mi>k</mi> </mfenced> </mrow> </semantics></math>: non-filtered and filtered for measured signals.</p>
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<p>Instantaneous power obtained using Equation (22) using measured signals.</p>
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<p>Evolution of the estimated average power using measured signals.</p>
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26 pages, 7114 KiB  
Article
Fault Diagnosis Method for Centrifugal Pumps in Nuclear Power Plants Based on a Multi-Scale Convolutional Self-Attention Network
by Chen Li, Xinkai Liu, Hang Wang and Minjun Peng
Sensors 2025, 25(5), 1589; https://doi.org/10.3390/s25051589 - 5 Mar 2025
Viewed by 92
Abstract
The health status of rotating machinery equipment in nuclear power plants is of paramount importance for ensuring the overall normal operation of the power plant system. In particular, significant failures in large rotating machinery equipment, such as main pumps, pose critical safety hazards [...] Read more.
The health status of rotating machinery equipment in nuclear power plants is of paramount importance for ensuring the overall normal operation of the power plant system. In particular, significant failures in large rotating machinery equipment, such as main pumps, pose critical safety hazards to the system. Therefore, this paper takes pump equipment as a representative of rotating machinery in nuclear power plants and proposes a fault diagnosis method based on a multi-scale convolutional self-attention network for three types of faults: outer ring fracture, inner ring fracture, and rolling element pitting corrosion. Within the multi-scale convolutional self-attention network, a multi-scale hybrid feature complementarity mechanism is introduced. This mechanism leverages an adaptive encoder to capture deep feature information from the acoustic signals of rolling bearings and constructs a hybrid-scale feature set based on deep features and original signal characteristics in the time–frequency domain. This approach enriches the fault information present in the feature set and establishes a nonlinear mapping relationship between fault features and rolling bearing faults. The results demonstrate that, without significantly increasing model complexity or the volume of feature data, this method achieves a substantial increase in fault diagnosis accuracy, exceeding 99.5% under both vibration signal and acoustic signal conditions. Full article
(This article belongs to the Section Physical Sensors)
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<p>Schematic diagram of the autoencoder structure.</p>
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<p>A fault diagnosis model based on the multi-scale convolutional self-attention mechanism Network.</p>
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<p>Overall design diagram of the experimental bench for the rolling bearing failure of a circulating water pump.</p>
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<p>Actual effect diagram of the experimental bench for the rolling bearing failure of a circulating water pump.</p>
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<p>Rolling bearing faulty parts. (<b>a</b>) Outer ring fracture fault; (<b>b</b>) Inner ring fracture fault; (<b>c</b>) Rolling element pitting fault.</p>
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<p>Layout of vibration signal measurement points for the circulating water pump.</p>
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<p>Layout of acoustic signal measurement points for the circulating water pump.</p>
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<p>The change curves of training loss, testing loss, training accuracy, and testing accuracy during 30 iterations of four fault diagnosis models by vibration signal: (<b>a</b>) CNN, (<b>b</b>) TCN, (<b>c</b>) CSA, and (<b>d</b>) MS-CSA.</p>
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<p>Confusion matrix of four fault diagnosis models by vibration signal: (<b>a</b>) CNN, (<b>b</b>) TCN, (<b>c</b>) CSA, and (<b>d</b>) MS-CSA.</p>
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<p>t-SNE of four fault diagnosis models by vibration signal: (<b>a</b>) CNN, (<b>b</b>) TCN, (<b>c</b>) CSA, and (<b>d</b>) MS-CSA.</p>
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<p>The change curves of training loss, testing loss, training accuracy, and testing accuracy during 30 iterations of four fault diagnosis models by acoustic signal: (<b>a</b>) CNN, (<b>b</b>) TCN, (<b>c</b>) CSA, and (<b>d</b>) MS-CSA.</p>
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<p>The change curves of training loss, testing loss, training accuracy, and testing accuracy during 30 iterations of four fault diagnosis models by acoustic signal: (<b>a</b>) CNN, (<b>b</b>) TCN, (<b>c</b>) CSA, and (<b>d</b>) MS-CSA.</p>
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<p>Confusion matrix of four fault diagnosis models by acoustic signal: (<b>a</b>) CNN, (<b>b</b>) TCN, (<b>c</b>) CSA, and (<b>d</b>) MS-CSA.</p>
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<p>t-SNE of four fault diagnosis models by acoustic signal: (<b>a</b>) CNN, (<b>b</b>) TCN, (<b>c</b>) CSA, and (<b>d</b>) MS-CSA.</p>
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<p>The fault diagnosis test platform of Case Western Reserve University.</p>
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<p>The change curves of training loss, testing loss, training accuracy, and testing accuracy during 30 iterations of four fault diagnosis models by general data: (<b>a</b>) CNN, (<b>b</b>) TCN, (<b>c</b>) CSA, and (<b>d</b>) MS-CSA.</p>
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<p>Confusion matrix of four fault diagnosis models by general data: (<b>a</b>) CNN, (<b>b</b>) TCN, (<b>c</b>) CSA, and (<b>d</b>) MS-CSA.</p>
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<p>t-SNE of four fault diagnosis models by general data: (<b>a</b>) CNN, (<b>b</b>) TCN, (<b>c</b>) CSA, and (<b>d</b>) MS-CSA.</p>
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17 pages, 5331 KiB  
Article
Noise Reduction of Steam Trap Based on SSA-VMD Improved Wavelet Threshold Function
by Shuxun Li, Qian Zhao, Jinwei Liu, Xuedong Zhang and Jianjun Hou
Sensors 2025, 25(5), 1573; https://doi.org/10.3390/s25051573 - 4 Mar 2025
Viewed by 130
Abstract
The performance of steam traps plays an important role in the normal operation of steam systems. It also contributes to the improvement of thermal efficiency of steam-using equipment and the rational use of energy. As an important component of the steam system, it [...] Read more.
The performance of steam traps plays an important role in the normal operation of steam systems. It also contributes to the improvement of thermal efficiency of steam-using equipment and the rational use of energy. As an important component of the steam system, it is crucial to monitor the state of the steam trap and establish a correlation between the acoustic emission signal and the internal leakage state. However, in actual test environments, the acoustic emission sensor often collects various background noises alongside the valve internal leakage acoustic emission signal. Therefore, to minimize the impact of environmental noise on valve internal leakage identification, it is necessary to preprocess the original acoustic emission signals through noise reduction before identification. To address the above problems, a denoising method based on a sparrow search algorithm, variational modal decomposition, and improved wavelet thresholding is proposed. The sparrow search algorithm, using minimum envelope entropy as the fitness function, optimizes the decomposition level K and the penalty factor α of the variational modal decomposition algorithm. This removes modes with higher entropy in the modal envelopes. Subsequently, wavelet threshold denoising is applied to the remaining modes, and the denoised signal is reconstructed. Validation analysis demonstrates that the combination of SSA-VMD and the improved wavelet threshold function effectively filters out noise from the signal. Compared to traditional thresholding methods, this approach increases the signal-to-noise ratio and reduces the root-mean-square error, significantly enhancing the noise reduction effect on the steam trap’s background noise signal. Full article
(This article belongs to the Section Physical Sensors)
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<p>Comparison of improved exponential threshold functions.</p>
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<p>Structural diagram of the steam trap used in the test.</p>
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<p>Steam trap signal collection experiment site diagram.</p>
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<p>The physical picture of the multi-channel high-frequency acoustic emission acquisition instrument.</p>
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<p>The pre-signal amplifier. The Chinese refers to the manufacturer of the preamplifier, whose English name is Beijing Ruandao Technology Co, Ltd.</p>
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<p>The actual picture of the acoustic emission sensor.</p>
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<p>The high vacuum coupling agent. The Chinese is the name of the coupling agent, and its English name is high vacuum silicone grease.</p>
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<p>The measured signal diagram of the steam trap valve.</p>
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<p>The decomposition parameter optimization curve.</p>
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<p>Time domain graphs after noise reduction. (<b>a</b>) The hard threshold function denoising time-domain graph; (<b>b</b>) The soft threshold function denoising time-domain graph; (<b>c</b>) The improved wavelet threshold function denoising time-domain graph; (<b>d</b>) Joint SSA-VMD and the improved wavelet threshold denoising time-domain graph.</p>
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<p>Time domain graphs after noise reduction. (<b>a</b>) The hard threshold function denoising time-domain graph; (<b>b</b>) The soft threshold function denoising time-domain graph; (<b>c</b>) The improved wavelet threshold function denoising time-domain graph; (<b>d</b>) Joint SSA-VMD and the improved wavelet threshold denoising time-domain graph.</p>
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16 pages, 4467 KiB  
Article
Mechanical Behaviour of Rock Samples with Burst Liability Under Different Pre-Cycling Thresholds
by Jianhang Chen, Banquan Zeng, Wuyan Xu, Kun Wang, Krzysztof Skrzypkowski, Krzysztof Zagórski, Anna Zagórska and Zbigniew Rak
Appl. Sci. 2025, 15(5), 2760; https://doi.org/10.3390/app15052760 - 4 Mar 2025
Viewed by 130
Abstract
To study the influence of the main roof period pressure on the instability mechanism of rock pillars with burst liability, the composite loading mode of “pre-cycling loading + continuous loading with a constant rate” was used to conduct compression experiments on rock samples. [...] Read more.
To study the influence of the main roof period pressure on the instability mechanism of rock pillars with burst liability, the composite loading mode of “pre-cycling loading + continuous loading with a constant rate” was used to conduct compression experiments on rock samples. Meanwhile, the mechanical behaviour response characteristics of rock samples were discussed. Experiment results are shown as follows: (1) mechanical properties of rock samples were strengthened by closing primary pores under pre-cycling loading. The surface roughness and secondary crack number decreased gradually with the pre-cycling threshold; (2) the Kaiser effect of AE (Acoustic Emission) signals was significant in the second and third pre-cycling loading and unloading stages. The Kaiser effect disappeared in the continuous loading stage; (3) AF-RA (Average Frequency-Risetime Amplitude) signals were distributed in a dense-sparse-dense form. Low AF and high RA shear type cracks were more common. Shear failure was the dominant failure mode in rock samples. Full article
(This article belongs to the Section Civil Engineering)
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<p>Experimental stress–strain curves.</p>
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<p>Experimental apparatus.</p>
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<p>Experimental loading mode.</p>
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<p>Stress–strain and peak stress evolution curves: (<b>a</b>) stress–strain curves of rock samples; (<b>b</b>) relationship between average peak stress and pre-cycling thresholds.</p>
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<p>Microstructure characteristics of rock samples with burst liability.</p>
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<p>AE signal characteristics of rock samples with burst liability: (<b>a</b>) AE count was 0–30 × 10<sup>4</sup> and the pre-cycling threshold was 6 MPa; (<b>b</b>) AE count was 0–0.06 × 10<sup>4</sup> and the pre-cycling threshold was 6 MPa; (<b>c</b>) AE count was 0–5 × 10<sup>4</sup> and the pre-cycling threshold was 12 MPa; (<b>d</b>) AE count was 0–0.06 × 10<sup>4</sup> and the pre-cycling threshold was 12 MPa; (<b>e</b>) AE count was 0–4 × 10<sup>4</sup> and the pre-cycling threshold was 18 MPa; (<b>f</b>) AE count was 0–0.06 × 10<sup>4</sup> and the pre-cycling threshold was 18 MPa.</p>
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<p>Evolution characteristics of the Kaiser effect: (<b>a</b>) pre-cycling threshold was 6 MPa; (<b>b</b>) pre-cycling threshold was 12 MPa; (<b>c</b>) pre-cycling threshold was 18 MPa.</p>
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<p>Relationship between <span class="html-italic">AF-RA</span> and crack type.</p>
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<p>Evolution characteristics of <span class="html-italic">AF-RA</span> and crack types: (<b>a</b>) Relationship between <span class="html-italic">AF-RA</span> and time when pre-cycling threshold was 6 MPa; (<b>b</b>) Relationship between <span class="html-italic">AF</span> and <span class="html-italic">RA</span> when pre-cycling threshold was 6 MPa; (<b>c</b>) Relationship between <span class="html-italic">AF-RA</span> and time when pre-cycling threshold was 12 MPa; (<b>d</b>) Relationship between <span class="html-italic">AF</span> and <span class="html-italic">RA</span> when pre-cycling threshold was 12 MPa; (<b>e</b>) Relationship between <span class="html-italic">AF-RA</span> and time when pre-cycling threshold was 18 MPa; (<b>f</b>) Relationship between <span class="html-italic">AF</span> and <span class="html-italic">RA</span> when pre-cycling threshold was 18 MPa.</p>
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16 pages, 1813 KiB  
Article
Innovative Regression Model for Frequency-Dependent Acoustic Source Strength in the Aquatic Environment: Bridging Scientific Insight and Practical Applications
by Moshe Greenberg, Uri Kushnir and Vladimir Frid
Sensors 2025, 25(5), 1560; https://doi.org/10.3390/s25051560 - 3 Mar 2025
Viewed by 373
Abstract
This study addresses the challenge of predicting acoustic source strength in freshwater environments, focusing on frequencies between 100–400 kHz. Acoustic signal attenuation is inherently frequency-dependent and influenced by water properties as well as the total propagation path of the acoustic wave, complicating the [...] Read more.
This study addresses the challenge of predicting acoustic source strength in freshwater environments, focusing on frequencies between 100–400 kHz. Acoustic signal attenuation is inherently frequency-dependent and influenced by water properties as well as the total propagation path of the acoustic wave, complicating the accurate determination of source strength. To address this challenge, we developed a non-linear regression model for solving the inverse problem of attenuation correction in reflected signals from typical aquatic reflectors, addressing the current absence of robust correction tools in this frequency range. The novelty of our approach lies in designing a non-linear regression framework that incorporates key physical parameters—signal energy, propagation distance, and frequency—enabling accurate source strength prediction. Using an experimental setup comprising ultrasonic transducers and a signal generator under controlled conditions, we collected a comprehensive dataset of 366 samples. The results demonstrate that our proposed model achieves reliable source strength prediction by simplifying Thorpe’s equation for freshwater environments. This research represents a significant advancement in underwater acoustics, providing a practical and reliable tool for source strength estimation in freshwater systems. The developed methodology may have broad applications across sonar technology, environmental monitoring, and aquatic research domains. Full article
(This article belongs to the Section Physical Sensors)
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<p>The experimental setup includes ultrasonic transducers (transmitter and receiver), a signal generator, a digital oscilloscope, a mechanical spacer (a bar), and a water tank.</p>
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<p>A schematic sketch for the experimental setup.</p>
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<p>The dimensions of the transducers (MISTRAS Group, West Windsor, NJ, USA).</p>
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<p>Transducer reception ranges in decibel values as a function of frequency. (MISTRAS Group, West Windsor, NJ, USA).</p>
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<p>Predicted vs. Measured values for regression model case 4: (<b>a</b>) Training set, (<b>b</b>) Test set.</p>
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15 pages, 8355 KiB  
Article
Data Acquisition and Chatter Recognition Based on Multi-Sensor Signals for Blade Whirling Milling
by Xinyu Li, Riliang Liu and Zhiying Zhu
Machines 2025, 13(3), 206; https://doi.org/10.3390/machines13030206 - 2 Mar 2025
Viewed by 225
Abstract
Bladed components are essential in engines and propulsion systems, but their thin structures, complex geometries, and significant material removal rates during machining make them challenging to manufacture. This study investigates the chatter phenomenon in blade whirling milling, a promising method for improving machining [...] Read more.
Bladed components are essential in engines and propulsion systems, but their thin structures, complex geometries, and significant material removal rates during machining make them challenging to manufacture. This study investigates the chatter phenomenon in blade whirling milling, a promising method for improving machining efficiency. Multi-sensor signals, including vibration and acoustic emission signals, are collected during roughing and finishing machining. Time-domain, frequency-domain, and time-frequency features are extracted, filtered, and fused using principal component analysis (PCA) to retain relevant information while ensuring computational efficiency. The features are then input into an MLGRU-based chatter recognition model, incorporating a self-attention mechanism (SAM) for enhanced performance. The experimental results show that the proposed model achieves an average recognition accuracy of 89.16%, with a response time within 0.4 s, reflecting its effectiveness and timeliness in chatter detection. The findings also validate that the blade edge regions are more prone to chatter, especially during rough machining, due to their lower rigidity and greater sensitivity to external excitations. Full article
(This article belongs to the Special Issue Advances in Noises and Vibrations for Machines)
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<p>Schematic of whirling milling for bladed components.</p>
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<p>Experimental setup for blade milling.</p>
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<p>Sampling schematic of the blade whirling milling process.</p>
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<p>Workpiece blank and formed blade.</p>
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<p>Flowchart of the signal acquisition experiment.</p>
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<p>Overall structure of the recognition model.</p>
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<p>Time-domain plots of signals.</p>
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<p>Frequency spectra of signals.</p>
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<p>Distribution of machining states for sampling segments and blade sections.</p>
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<p>Performance of the chatter recognition model on the experimental dataset.</p>
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27 pages, 4959 KiB  
Article
Deep Learning Autoencoders for Fast Fourier Transform-Based Clustering and Temporal Damage Evolution in Acoustic Emission Data from Composite Materials
by Serafeim Moustakidis, Konstantinos Stergiou, Matthew Gee, Sanaz Roshanmanesh, Farzad Hayati, Patrik Karlsson and Mayorkinos Papaelias
Infrastructures 2025, 10(3), 51; https://doi.org/10.3390/infrastructures10030051 - 2 Mar 2025
Viewed by 404
Abstract
Structural health monitoring (SHM) in fiber-reinforced polymer (FRP) composites is essential to ensure safety and reliability during service, particularly in critical industries such as aerospace and wind energy. Traditional methods of analyzing Acoustic Emission (AE) signals in the time domain often fail to [...] Read more.
Structural health monitoring (SHM) in fiber-reinforced polymer (FRP) composites is essential to ensure safety and reliability during service, particularly in critical industries such as aerospace and wind energy. Traditional methods of analyzing Acoustic Emission (AE) signals in the time domain often fail to accurately detect subtle or early-stage damage, limiting their effectiveness. The present study introduces a novel approach that integrates frequency-domain analysis using the fast Fourier transform (FFT) with deep learning techniques for more accurate and proactive damage detection. AE signals are first transformed into the frequency domain, where significant frequency components are extracted and used as inputs to an autoencoder network. The autoencoder model reduces the dimensionality of the data while preserving essential features, enabling unsupervised clustering to identify distinct damage states. Temporal damage evolution is modeled using Markov chain analysis to provide insights into how damage progresses over time. The proposed method achieves a reconstruction error of 0.0017 and a high R-squared value of 0.95, indicating the autoencoder’s effectiveness in learning compact representations while minimizing information loss. Clustering results, with a silhouette score of 0.37, demonstrate well-separated clusters that correspond to different damage stages. Markov chain analysis captures the transitions between damage states, providing a predictive framework for assessing damage progression. These findings highlight the potential of the proposed approach for early damage detection and predictive maintenance, which significantly improves the effectiveness of AE-based SHM systems in reducing downtime and extending component lifespan. Full article
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<p>High-level architecture of the proposed methodology.</p>
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<p>Sensor positions for the tensile test (<b>left</b>) and 3-point bend (<b>right</b>).</p>
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<p>Raw acoustic data captured from a sample strip in the 3-point bending machine: (<b>a</b>) the whole duration of the experiment; (<b>b</b>) a zoomed-in visualization of a single AE event.</p>
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<p>Preprocessing pipeline for AE data, including noise removal, DC offset correction, segmentation, and frequency-domain transformation using <span class="html-italic">FFT</span>.</p>
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<p>Comparative literature values for the frequency ranges of damage in CFRPs. Data adapted from [<a href="#B25-infrastructures-10-00051" class="html-bibr">25</a>,<a href="#B27-infrastructures-10-00051" class="html-bibr">27</a>,<a href="#B28-infrastructures-10-00051" class="html-bibr">28</a>,<a href="#B29-infrastructures-10-00051" class="html-bibr">29</a>], illustrating variations in reported frequency bands for matrix cracking, delamination, debonding, fiber breakage, and fiber pull-out.</p>
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<p>Examples of Peak Frequency Assessment of a Tensile Tested CFRP Sample Coupon; (<b>a</b>) Time vs. Peak Frequency and (<b>b</b>) Magnitude vs. Peak Frequency.</p>
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<p>Time- and frequency-domain AE signals: (<b>a</b>–<b>c</b>) data with a detected AE event; (<b>d</b>) data without a detected AE event. DC offset has been removed from the time domain signals.</p>
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<p>Thresholding on the frequency domain (mean <span class="html-italic">FFT</span>) for detection of events (example from lab experiment).</p>
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<p>Bayesian optimization convergence.</p>
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<p>Examples of reconstructed and original <span class="html-italic">FFT</span> signals.</p>
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<p>Analysis of the mean frequency content of two clusters over time. The top plot shows the evolution of the mean frequency content for Cluster 1 and Cluster 2 with accumulated mean frequency curves. The bottom plots display the normalized amplitude of the mean frequency signals for Cluster 1 (<b>left</b>) and Cluster 2 (<b>right</b>), highlighting distinct peaks at specific frequencies within each cluster (results for lab experiment).</p>
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<p>State transition diagram (Markov chain) representing the probability of transitioning between two clusters. The diagram shows self-transition probabilities for Cluster 1 and Cluster 2, as well as the transition probabilities between the two clusters. The width of the arrows is proportional to the transition probabilities, with values indicated along each transition path.</p>
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20 pages, 5438 KiB  
Article
Separation of Simultaneous Speakers with Acoustic Vector Sensor
by Józef Kotus and Grzegorz Szwoch
Sensors 2025, 25(5), 1509; https://doi.org/10.3390/s25051509 - 28 Feb 2025
Viewed by 126
Abstract
This paper presents a method of sound source separation in live audio signals, based on sound intensity analysis. Sound pressure signals recorded with an acoustic vector sensor are analyzed, and the spectral distribution of sound intensity in two dimensions is calculated. Spectral components [...] Read more.
This paper presents a method of sound source separation in live audio signals, based on sound intensity analysis. Sound pressure signals recorded with an acoustic vector sensor are analyzed, and the spectral distribution of sound intensity in two dimensions is calculated. Spectral components of the analyzed signal are selected based on the calculated source direction, which leads to a spatial filtration of the sound. The experiments were performed with test signals convolved with impulse responses of a real sensor, recorded for a varying sound source position. The experiments evaluated the proposed method’s ability to separate sound sources, depending on their position, spectral content, and signal-to-noise ratio, especially when multiple sources are active at the same time. The obtained results are presented and discussed. The proposed algorithm provided signal-to-distortion ratio (SDR) values 10–12 dB, and Short-Time Objective Intelligibility Measure (STOI) values in the range 0.86–0.94, an increase by 0.15–0.30 compared with the unprocessed speech signal. The proposed method is intended for applications in automated speech recognition systems, speaker diarization, and separation in the concurrent speech scenarios, using a small acoustic sensor. Full article
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<p>Block diagram of the proposed algorithm for the separation of the desired signal from the disturbance.</p>
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<p>Example spectrograms: (<b>a</b>) input signal to the algorithm—male speech <span class="html-italic">x<sub>s</sub></span> at 0° mixed with the disturbance <span class="html-italic">x<sub>n</sub></span> (female speech) at 30°, (<b>b</b>) the processing result <span class="html-italic">y<sub>s</sub></span>, and (<b>c</b>) the original signal <span class="html-italic">x<sub>s</sub></span>. Color represents the spectral magnitude level in dB.</p>
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<p>Example of the signal processing: a binary spectral mask. Black color denotes spectral components that are removed from the signal.</p>
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<p>SDR values calculated between the input <span class="html-italic">x<sub>s</sub></span> and the output <span class="html-italic">y<sub>s</sub></span> signals, for a varying angular distance between the sources. Three combinations of female (F) and male (M) voices are presented.</p>
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<p>SDR values calculated for a varying azimuth range of interest for the desired signal for the M-F case (M source at 0°, F source at 90°, equal SNR).</p>
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<p>STOI difference between the processed and the unprocessed signal, for a varying angular distance between the sources.</p>
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<p>PESQ values calculated for a varying angular distance between the sources.</p>
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<p>SDR values calculated for a varying input SNR (source distance = 45°).</p>
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<p>STOI results calculated for a varying input SNR (source distance = 45°): (<b>a</b>) STOI values, and (<b>b</b>) the difference between the STOI for the processed and the unprocessed signal.</p>
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17 pages, 2199 KiB  
Systematic Review
Artificial Intelligence-Driven Wireless Sensing for Health Management
by Merih Deniz Toruner, Victoria Shi, John Sollee, Wen-Chi Hsu, Guangdi Yu, Yu-Wei Dai, Christian Merlo, Karthik Suresh, Zhicheng Jiao, Xuyu Wang, Shiwen Mao and Harrison Bai
Bioengineering 2025, 12(3), 244; https://doi.org/10.3390/bioengineering12030244 - 27 Feb 2025
Viewed by 318
Abstract
(1) Background: With technological advancements, the integration of wireless sensing and artificial intelligence (AI) has significant potential for real-time monitoring and intervention. Wireless sensing devices have been applied to various medical areas for early diagnosis, monitoring, and treatment response. This review focuses on [...] Read more.
(1) Background: With technological advancements, the integration of wireless sensing and artificial intelligence (AI) has significant potential for real-time monitoring and intervention. Wireless sensing devices have been applied to various medical areas for early diagnosis, monitoring, and treatment response. This review focuses on the latest advancements in wireless, AI-incorporated methods applied to clinical medicine. (2) Methods: We conducted a comprehensive search in PubMed, IEEEXplore, Embase, and Scopus for articles that describe AI-incorporated wireless sensing devices for clinical applications. We analyzed the strengths and limitations within their respective medical domains, highlighting the value of wireless sensing in precision medicine, and synthesized the literature to provide areas for future work. (3) Results: We identified 10,691 articles and selected 34 that met our inclusion criteria, focusing on real-world validation of wireless sensing. The findings indicate that these technologies demonstrate significant potential in improving diagnosis, treatment monitoring, and disease prevention. Notably, the use of acoustic signals, channel state information, and radar emerged as leading techniques, showing promising results in detecting physiological changes without invasive procedures. (4) Conclusions: This review highlights the role of wireless sensing in clinical care and suggests a growing trend towards integrating these technologies into routine healthcare, particularly patient monitoring and diagnostic support. Full article
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<p>Literature search and selection process in this study.</p>
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<p>Study characteristics. (<b>A</b>) Distributions of publication year of the studies. (<b>B</b>) Distributions of country of origin of the first author in included studies.</p>
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<p>Medical areas of selected studies.</p>
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21 pages, 4009 KiB  
Article
Applying Acoustic Signals to Monitor Hybrid Electrical Discharge-Turning with Artificial Neural Networks
by Mehdi Soleymani and Mohammadjafar Hadad
Micromachines 2025, 16(3), 274; https://doi.org/10.3390/mi16030274 - 27 Feb 2025
Viewed by 147
Abstract
Artificial intelligence (AI) models have demonstrated their capabilities across various fields by performing tasks that are currently handled by humans. However, the training of these models faces several limitations, such as the need for sufficient data. This study proposes the use of acoustic [...] Read more.
Artificial intelligence (AI) models have demonstrated their capabilities across various fields by performing tasks that are currently handled by humans. However, the training of these models faces several limitations, such as the need for sufficient data. This study proposes the use of acoustic signals as training data as this method offers a simpler way to obtain a large dataset compared to traditional approaches. Acoustic signals contain valuable information about the process behavior. We investigated the ability of extracting useful features from acoustic data expecting to predict labels separately by a multilabel classifier rather than as a multiclass classifier. This study focuses on electrical discharge turning (EDT) as a hybrid process of electrical discharge machining (EDM) and turning, an intricate process with multiple influencing parameters. The sounds generated during EDT were recorded and used as training data. The sounds underwent preprocessing to examine the effects of the parameters used for feature extraction prior to feeding the data into the ANN model. The parameters investigated included sample rate, length of the FFT window, hop length, and the number of mel-frequency cepstral coefficients (MFCC). The study aimed to determine the optimal preprocessing parameters considering the highest precision, recall, and F1 scores. The results revealed that instead of using the default set values in the python packages, it is necessary to investigate the preprocessing parameters to find the optimal values for the maximum classification performance. The promising results of the multi-label classification model depicted that it is possible to detect various aspects of a process simultaneously receiving single data, which is very beneficial in monitoring. The results also indicated that the highest prediction scores could be achieved by setting the sample rate, length of the FFT window, hop length, and number of MFCC to 4500 Hz, 1024, 256, and 80, respectively. Full article
(This article belongs to the Special Issue Future Prospects of Additive Manufacturing)
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<p>EDT setup, the driver and controller, and the recording device applied for machining and signal recording.</p>
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<p>Scanning Electron Microscope images from the machined surface.</p>
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<p>Schematic of windows and the segmenting of frames.</p>
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<p>Schematic of feature extraction and the ANN architecture in which each hidden layer has a different color and each tick mark is the representative of the selected label.</p>
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<p>Accuracy diagrams for different sample rates (sr) and numbers of fft (n_fft).</p>
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<p>Accuracy diagrams for different numbers of MFCC (n_mfcc) and hop length.</p>
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21 pages, 4815 KiB  
Article
Effective Strategies for Automatic Analysis of Acoustic Signals in Long-Term Monitoring
by Dídac Diego-Tortosa, Danilo Bonanno, Manuel Bou-Cabo, Letizia S. Di Mauro, Abdelghani Idrissi, Guillermo Lara, Giorgio Riccobene, Simone Sanfilippo and Salvatore Viola
J. Mar. Sci. Eng. 2025, 13(3), 454; https://doi.org/10.3390/jmse13030454 - 27 Feb 2025
Viewed by 211
Abstract
Hydrophones used in Passive Acoustic Monitoring generate vast amounts of data, with the storage requirements for raw signals dependent on the sampling frequency, which limits the range of frequencies that can be recorded. Since the installation of these observatories is costly, it is [...] Read more.
Hydrophones used in Passive Acoustic Monitoring generate vast amounts of data, with the storage requirements for raw signals dependent on the sampling frequency, which limits the range of frequencies that can be recorded. Since the installation of these observatories is costly, it is crucial to maximize the utility of high-sampling-rate recordings to expand the range of survey types. However, storing these large datasets for long-term trend analysis presents significant challenges. This paper proposes an approach that reduces the data storage requirements by up to 85% while preserving critical information about Power Spectral Density and Sound Pressure Level. The strategy involves generating these key metrics from spectrograms, enabling both short-term (micro) and long-term (macro) studies. A proposal for efficient data processing is presented, structured in three steps: the first focuses on generating key metrics to replace space-consuming raw signals, the second addresses the treatment of these metrics for long-term studies, and the third outlines the creation of event detectors from the processed metrics. A comprehensive overview of the essential features for analyzing acoustic signals is provided, along with considerations for the future design of marine observatories. The necessary calculations and processes are detailed, demonstrating the potential of these methods to address the current data storage and processing limitations in long-term acoustic monitoring. Full article
(This article belongs to the Special Issue Marine Environmental Noise)
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<p>Spectrogram notes to understand its characteristics and different metrics.</p>
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<p>Proposed space-saving workflow for long-term acoustic monitoring data.</p>
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<p><math display="inline"><semantics> <mrow> <mi>P</mi> <mi>L</mi> <mi>O</mi> <mi>T</mi> </mrow> </semantics></math>s representing the <math display="inline"><semantics> <mrow> <mi>P</mi> <mi>S</mi> <mi>D</mi> <mspace width="4pt"/> <mi>d</mi> <mi>a</mi> <mi>t</mi> <mi>a</mi> </mrow> </semantics></math> in the (<b>a</b>) high-frequency analysis and in the (<b>b</b>) low-frequency analysis. The black dashed line at 800 Hz indicates the maximum reliable frequency, beyond which the effects of the anti-aliasing filter occur.</p>
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<p><math display="inline"><semantics> <mrow> <mi>P</mi> <mi>L</mi> <mi>O</mi> <mi>T</mi> </mrow> </semantics></math>s representing the <math display="inline"><semantics> <mrow> <mi>P</mi> <mi>S</mi> <mi>D</mi> <mspace width="4pt"/> <mi>d</mi> <mi>a</mi> <mi>t</mi> <msub> <mi>a</mi> <mrow> <mi>c</mi> <mi>u</mi> <mi>m</mi> </mrow> </msub> </mrow> </semantics></math> in the (<b>a</b>) high-frequency analysis and in the (<b>b</b>) low-frequency analysis. The black dashed line at 800 Hz indicates the maximum reliable frequency, beyond which the effects of the anti-aliasing filter occur.</p>
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<p><math display="inline"><semantics> <mrow> <mi>P</mi> <mi>L</mi> <mi>O</mi> <mi>T</mi> </mrow> </semantics></math>s representing the <math display="inline"><semantics> <mrow> <mi>S</mi> <mi>P</mi> <mi>L</mi> <mspace width="4pt"/> <mi>d</mi> <mi>a</mi> <mi>t</mi> <mi>a</mi> </mrow> </semantics></math> in the (<b>a</b>) high-frequency analysis and in the (<b>b</b>) low-frequency analysis.</p>
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<p><math display="inline"><semantics> <mrow> <mi>P</mi> <mi>L</mi> <mi>O</mi> <mi>T</mi> </mrow> </semantics></math>s representing the <math display="inline"><semantics> <mrow> <mi>S</mi> <mi>P</mi> <mi>L</mi> <mspace width="4pt"/> <mi>d</mi> <mi>a</mi> <mi>t</mi> <msub> <mi>a</mi> <mrow> <mi>c</mi> <mi>u</mi> <mi>m</mi> </mrow> </msub> </mrow> </semantics></math> in the (<b>a</b>) high-frequency analysis and in the (<b>b</b>) low-frequency analysis.</p>
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<p>The proposed 24 h full spectrogram for long-term monitoring. The black dashed line at 800 Hz indicates the maximum reliable frequency, beyond which aliasing occurs in the low-frequency analysis. Note that the Y-axis extends to 100 kHz for visualization purposes, although the actual data are limited to 97.65625 kHz. The logarithmic scale reduces the apparent gap.</p>
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<p>A proposed heatmap representing the <math display="inline"><semantics> <mrow> <mi>S</mi> <mi>P</mi> <msub> <mi>L</mi> <mrow> <mn>25</mn> <mo>%</mo> </mrow> </msub> </mrow> </semantics></math> (5–100 Hz) for each hour over 60 days of recording. Days marked in red indicate Saturdays and Sundays.</p>
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<p>SPL full representation proposed to visualize the <math display="inline"><semantics> <mrow> <mi>S</mi> <mi>P</mi> <mi>L</mi> </mrow> </semantics></math> metrics between 5 and 100 Hz for each hour over 16 days of recording. The gray background is used to indicate Saturdays and Sundays.</p>
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<p>Representation of the <math display="inline"><semantics> <mrow> <mi>S</mi> <mi>P</mi> <msub> <mi>L</mi> <mrow> <mi>s</mi> <mi>u</mi> <mi>m</mi> <mo>.</mo> </mrow> </msub> </mrow> </semantics></math> for the third-octave bands up to 31.5 Hz in gray and the filtered wave in black. The Signal-to-Noise Ratio (SNR) of the peak that meets the detection criteria is displayed.</p>
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<p><math display="inline"><semantics> <mrow> <mi>P</mi> <mi>S</mi> <mi>D</mi> <mspace width="4pt"/> <mi>d</mi> <mi>a</mi> <mi>t</mi> <msub> <mi>a</mi> <mrow> <mi>c</mi> <mi>u</mi> <mi>m</mi> </mrow> </msub> </mrow> </semantics></math> representation for both low-frequency and high-frequency analyses of <a href="#jmse-13-00454-f007" class="html-fig">Figure 7</a>. The black dashed line at 800 Hz indicates the maximum reliable frequency, beyond which the effects of the anti-aliasing filter occur.</p>
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17 pages, 4042 KiB  
Article
Detecting Excitations of Pipes, Ropes, and Bars Using Piezo Sensors and Collecting Information Remotely
by Matteo Cirillo, Enzo Reali and Giuseppe Soda
Sensors 2025, 25(5), 1444; https://doi.org/10.3390/s25051444 - 27 Feb 2025
Viewed by 249
Abstract
An investigation of a non-invasive method to detect defects and localize excitations in metallic structures is presented. It is shown how signals generated by very sensitive piezo sensor assemblies, secured to the metallic elements, can allow for space localization of excitations and defects [...] Read more.
An investigation of a non-invasive method to detect defects and localize excitations in metallic structures is presented. It is shown how signals generated by very sensitive piezo sensor assemblies, secured to the metallic elements, can allow for space localization of excitations and defects in the analyzed structures. The origin of the piezo excitations are acoustic modes generated by light percussive excitations whose strength is of the order of tenths of a newton and that provide piezo signal amplitudes of a few hundred millivolts. Tests of the detection scheme of the excitations are performed on steel ropes, iron pipes, and bars with lengths in the range of 1–6 m with the sensor output signal shaped in the form of a clean pulse. It is shown that the signals generated by the piezo assemblies, when adequately shaped, can feed the input of an RF transmitter, which in turn transfers information to a remote receiver whose readout allows for remotely analyzing information collected on the metallic elements. Considering the voltage amplitude of the signals (of the order of 300 mV) generated by the piezo sensors as a result of very light percussive excitations, the low power required for transmitting data, and the low cost of the sensing and transmitting assembly, it is conceivable that our devices could detect excitations generated even tens of kilometers away and allow for setting up an array of sensors for controlling in real time the status of pipe networks. Full article
(This article belongs to the Special Issue Energy Harvesting and Self-Powered Sensors)
Show Figures

Figure 1

Figure 1
<p>Views of our sensor assembly. (<b>a</b>) Image of the top showing the piezo element, the fixers, and the screws securing those to a PCB; (<b>b</b>) the back of the PCB showing the end of the screws; (<b>c</b>) cross-section of the sensor assembly positioned on a 0.23 m-diameter pipe—below the sensor case three fixing screws contact the “transmitting plate”. The strong magnet (B = 0.45 T) fixes the plate to the pipe and robust tape (indicated by side) secures the case to the transmitting plate.</p>
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<p>(<b>a</b>) Photo of the hollow pipe on which we first tested our sensor assembly. The pipe, white in color, was held by two supports at its ends. The pipe length was 5.5 m, its diameter was 0.3 m, and its thickness was 0.01 m; (<b>b</b>) sensor response: negative values of the horizontal scale refer to the time before the sensor responded to the excitation, which is zero on the scale.</p>
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<p>Traces of the signal detected on a multichannel scope by our piezo sensor before (upper, green trace) and after the treatment transformed it into an 18 ms pulse ready to be conveyed to a transmitter (lower, violet trace). Vertical scales are 200 mV/div for the upper trace and 2 V/div for the lower trace.</p>
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<p>Flow chart of the system we have set up in order to transmit in the ether the signal generated by the piezoelectric sensor.</p>
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<p>In the upper panel, (<b>a</b>) we see the two transmitter and receiver boards in the transreceiver configuration; one is set in the “Sending Packet” mode, the other in the “Receiving Packet” mode. The lower panel (<b>b</b>) shows typical computer displays tracing the activity of the boards.</p>
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<p>(<b>a</b>) Sketch of the protocol for measuring the time it takes for an acoustic excitation to cover the space between the two sensors; (<b>b</b>) bare oscilloscope display of the consequence of the process.</p>
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<p>(<b>a</b>) Dependence of the time delays between the pulses generated by two sensor assemblies on the 6 meter-long pipe. The inset shows a photo of the cross-section of sensor positioning with the long side of the transmitting plate parallel to the pipe; (<b>b</b>) low-frequency spectrum showing the component corresponding to the fundamental frequency of the vibrating string model.</p>
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<p>(<b>a</b>) Time delays between sensor signals placed at different distances on an iron bar. The inset shows the bar surface. (<b>b</b>) Low-frequency spectrum (portion) of the excitations of the bar.</p>
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<p>(<b>a</b>) The time delays between the 4 m-long rope. The inset shows a section of the seven wire rope. (<b>b</b>) The spectrum of a 1 m-long rope, consistent with the propagation velocity determined from the time delay measurements.</p>
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<p>(<b>a</b>) Sketch of the experiments performed for detecting time delays between piezos. (<b>b</b>) Delay of the origin of the pulses detected by the sensors assemblies secured at a relative distance of 2.86 m, visualized on a multichannel oscilloscope, when a light percussive excitation is generated at one end. (<b>c</b>) Time delay when percussion is applied at equal distance between the piezo assemblies. Vertical scales are same for the two traces in (<b>b</b>,<b>c</b>).</p>
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<p>Time delay (2.1 ms) measured when the two sensors are on the sides of a defect represented by a strong magnet holding the ropes together (see photo).</p>
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<p>(<b>a</b>) Time delay between sensors placed 2 cm away from a 1.41 m-long steel bar as a consequence of a parallel excitation. (<b>b</b>) Time delay in the same positioning of the sensors in (<b>a</b>) when an artificial defect is introduced.</p>
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