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19 pages, 50647 KiB  
Article
Long-Pulse Thermography Application for Detection and Localisation of Embedded Optical Fibres into Glass Fibre Composite
by Katarzyna Majewska and Magdalena Mieloszyk
Materials 2024, 17(24), 6255; https://doi.org/10.3390/ma17246255 - 21 Dec 2024
Viewed by 380
Abstract
Composites have found applications in critical components and require a high degree of safety and reliability. To ensure this, structural health monitoring systems based on optical fibres embedded within structures are installed for continuous monitoring. Infrared thermography is a non-destructive method that can [...] Read more.
Composites have found applications in critical components and require a high degree of safety and reliability. To ensure this, structural health monitoring systems based on optical fibres embedded within structures are installed for continuous monitoring. Infrared thermography is a non-destructive method that can be applied to inspect the internal structure after manufacturing and during operation. This paper presents an application of pulsed thermography for observing and evaluating the internal structure of glass fibre-reinforced polymer samples with different arrangements of embedded optical fibres. The goal of the paper is to study the feasibility of using pulsed thermography to distinguish optical fibres from glass textile fibre bundles, as well as to track the arrangement of the optical fibres. Full article
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Figure 1
<p>Geometry of semi-infinite material with included cylinder- or sphere-based object.</p>
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<p>Mutual arrangement of the glass fibre bundle and optical fibres.</p>
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<p>(<b>a</b>) Photos, (<b>b</b>) schemes of samples, (<b>c</b>) schema and photo of set-up.</p>
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<p>(<b>a</b>) Photos, (<b>b</b>) schemes of samples, (<b>c</b>) schema and photo of set-up.</p>
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<p>Timing graphs for two different arrangements of OFs with analysed frames (I–V): (<b>a</b>) arrangement OFs ‘+’, (<b>b</b>) arrangement OFs ‘x’.</p>
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<p>An example of OFs arrangement presented in the form of graphical visualisation of matrix <span class="html-italic">P</span>.</p>
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<p>Exemplary frames: without ‘0’, after typical ‘t’, proposed ‘p’, and combination ‘c’ of typical and proposed signal filtering methods applied for both arrangements (‘+’, ‘x’) for case B (both lamps).</p>
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<p>Analysed frame ‘V’: without ‘0’, after typical ‘t’, proposed ‘p’, and combination ‘c’ of typical and proposed signal filtering methods applied for case B (both lamps), L (left lamp), R (right lamp).</p>
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<p>Analysed frame ‘V’: without ‘0’, after typical ‘t’, proposed ‘p’, and combination ‘c’ of typical and proposed signal filtering methods applied for case B (both lamps), L (left lamp), R (right lamp).</p>
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<p>Comparison of the results for ‘+’ case.</p>
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<p>Comparison of the results for ‘x’ case.</p>
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<p>Analysed frame ‘I’: without ‘0’, after typical ‘t’, proposed ‘p’, and combination ‘c’ of typical and proposed signal filtering methods applied for case B (both lamps), L (left lamp), R (right lamp).</p>
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<p>Analysed frame ‘II’: without ‘0’, after typical ‘t’, proposed ‘p’, and combination ‘c’ of typical and proposed signal filtering methods applied for case B (both lamps), L (left lamp), R (right lamp).</p>
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<p>Analysed frame ‘III’: without ‘0’, after typical ‘t’, proposed ‘p’, and combination ‘c’ of typical and proposed signal filtering methods applied for case B (both lamps), L (left lamp), R (right lamp).</p>
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<p>Analysed frame ‘IV’: without ‘0’, after typical ‘t’, proposed ‘p’, and combination ‘c’ of typical and proposed signal filtering methods applied for case B (both lamps), L (left lamp), R (right lamp).</p>
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<p>Analysed frame ‘I’: without ‘0’, after typical ‘t’, proposed ‘p’, and combination ‘c’ of typical and proposed signal filtering methods applied for case B (both lamps), L (left lamp), R (right lamp).</p>
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<p>Analysed frame ‘II’: without ‘0’, after typical ‘t’, proposed ‘p’, and combination ‘c’ of typical and proposed signal filtering methods applied for case B (both lamps), L (left lamp), R (right lamp).</p>
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<p>Analysed frame ‘III’: without ‘0’, after typical ‘t’, proposed ‘p’, and combination ‘c’ of typical and proposed signal filtering methods applied for case B (both lamps), L (left lamp), R (right lamp).</p>
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<p>Analysed frame ‘IV’: without ‘0’, after typical ‘t’, proposed ‘p’, and combination ‘c’ of typical and proposed signal filtering methods applied for case B (both lamps), L (left lamp), R (right lamp).</p>
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20 pages, 9659 KiB  
Article
Nondestructive Detection of Osmotic Damage in GFRP Boat Hulls Using Active Infrared Thermography Methods
by Endri Garafulić, Petra Bagavac and Lovre Krstulović-Opara
J. Mar. Sci. Eng. 2024, 12(12), 2247; https://doi.org/10.3390/jmse12122247 - 6 Dec 2024
Viewed by 424
Abstract
This article presents the application of infrared thermography as a nondestructive testing method (NDT) for detecting osmotic damage in glass-fiber-reinforced polymer (GFRP) and glass-reinforced polymer (GRP) boat hull structures. The aim of the conducted experiments is to explore the possibilities of applying active [...] Read more.
This article presents the application of infrared thermography as a nondestructive testing method (NDT) for detecting osmotic damage in glass-fiber-reinforced polymer (GFRP) and glass-reinforced polymer (GRP) boat hull structures. The aim of the conducted experiments is to explore the possibilities of applying active infrared thermography to real structures and to establish a procedure capable of filtering out anomalies caused by various thermal influences, such as thermal reflections from surrounding objects, geometry effects, and heat flow variations on the observed object. The methods used for post-processing IR signals include lock-in thermography (LT), pulse thermography (PT), pulse phase thermography (PPT), and gradient pulse phase thermography (GT). The practical application and advantages and disadvantages of infrared thermography in identifying osmotic damage in GFRP and GRP boat hulls will be illustrated through three case studies. Each case study is based on specific conditions and characteristics of different types of osmotic damage, enabling a thorough analysis of the effectiveness of the method in detecting and assessing the severity of the damage. The post-processed thermal images enable a clearer distinction between damaged and undamaged zones, improving the robustness of detection under realistic field conditions. Full article
(This article belongs to the Section Ocean Engineering)
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Figure 1
<p>Formation of osmotic bubbles.</p>
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<p>(<b>a</b>) Visible blisters and (<b>b</b>) the standard method of detecting the osmotic process.</p>
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<p>The transition from the (<b>a</b>) time domain to the (<b>b</b>) frequency domain using the FFT algorithm [<a href="#B14-jmse-12-02247" class="html-bibr">14</a>].</p>
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<p>Signal processing in PPT: (<b>a</b>) thermogram sequence, 3D matrix, and thermal profiles for a defective pixel, red line (Td), a nondefective pixel, blue line (TSa), and the difference between them, green line (TdTSa); (<b>b</b>) amplitudegram sequence and amplitude profiles; (<b>c</b>) phasegram sequence and phase profiles for a defective pixel, red line (Fd), a non-defective pixel, blue line (Fsa), and the difference between them, green line (Fd-Fsa).</p>
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<p>(<b>a</b>) Setup for nondestructive testing with lock-in thermography, (<b>b</b>) region of interest (ROI) where osmotic damage is circled and marked with labels A, B, C, and D.</p>
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<p>Sinusoidal response of relay-controlled halogen floodlights.</p>
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<p>Raw thermal image.</p>
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<p>Phase delay, P = 24 s, the osmotic damage is circled and marked with labels A, B, C, and D.</p>
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<p>Phase delay, P = 72 s, the osmotic damage is circled and marked with labels A, B, C, and D.</p>
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<p>Phase delay, P = 120 s, the osmotic damage is circled and marked with labels A, B, C, and D.</p>
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<p>Osmotic damage on the boat hull: (<b>a</b>) photo of the boat hull, (<b>b</b>) osmotic blisters A and B.</p>
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<p>A-scan of the back wall on calibration steel block K1: (<b>a</b>) 4 MHz frequency probe, (<b>b</b>) 1 MHz frequency probe.</p>
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<p>(<b>a</b>) USM GO device; (<b>b</b>) K1S-C 1 MHz frequency probe with a plexiglass attachment for beam focusing.</p>
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<p>A-scan: (<b>a</b>) osmotic damage, (<b>b</b>) undamaged material.</p>
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<p>Phase shift at different excitation frequencies: (<b>a</b>) f = 0.04167 Hz, (<b>b</b>) f = 0.0208 Hz, (<b>c</b>) f = 0.0139 Hz, and (<b>d</b>) f = 0.0083 Hz.</p>
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<p>Phase shift at different excitation frequencies: (<b>a</b>) f = 0.04167 Hz, (<b>b</b>) f = 0.0208 Hz, (<b>c</b>) f = 0.0139 Hz, and (<b>d</b>) f = 0.0083 Hz.</p>
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<p>Osmotic damage on the hull of the vessel after grinding the anti-fouling paint and protective epoxy coating.</p>
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<p>The undamaged hull of the vessel: (<b>a</b>) during UT testing, (<b>b</b>) after grinding the anti-fouling paint and protective epoxy coating.</p>
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<p>Phase shift at different excitation frequencies: (<b>a</b>) f = 0.04167 Hz, (<b>b</b>) f = 0.0208 Hz, (<b>c</b>) f = 0.0139 Hz, and (<b>d</b>) f = 0.0083 Hz.</p>
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<p>(<b>a</b>) PT applied on a boat’s hull, (<b>b</b>) photography of zones where blisters are detected, and (<b>c</b>) thermogram with location of osmotic blisters.</p>
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<p>PPT results of blister osmosis detection: (<b>a</b>) selected amplitudegrams—even symmetry; (<b>b</b>) selected phasegrams—odd symmetry, for the following frequencies: ±0.01, 0.02, 0.03, 0.04, 0.05 Hz.</p>
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<p>Boat’s hull phasegrams, image detail of osmosis damage—2D review for (<b>a</b>) f = 0.01 Hz and (<b>c</b>) f = 0.075 Hz, and 3D review for (<b>b</b>) f = 0.01 Hz and (<b>d</b>) f = 0.075 Hz.</p>
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<p>(<b>a</b>) Thermogram with the location of the osmotic blisters, (<b>b</b>) and thermal gradient image processing.</p>
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<p>Gradient of phasegram image shown in <a href="#jmse-12-02247-f022" class="html-fig">Figure 22</a>a.</p>
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<p>Wet fiberglass and delamination from the acids in zone A.</p>
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15 pages, 5185 KiB  
Article
Thermal and Structural Analysis of a High-Entropy Cr16Mn16Fe16Co16Ni16P20 Alloy—Influence of Cooling Rates on Phase Transformations
by Krzysztof Ziewiec, Artur Błachowski, Krystian Prusik, Marcin Jasiński, Aneta Ziewiec and Mirosława Wojciechowska
Materials 2024, 17(23), 5772; https://doi.org/10.3390/ma17235772 - 25 Nov 2024
Viewed by 525
Abstract
This study investigates the influence of cooling rates on the microstructure and phase transformations of the high-entropy alloy Cr16Mn16Fe16Co16Ni16P20. The alloy was synthesized via arc melting and subjected to three cooling [...] Read more.
This study investigates the influence of cooling rates on the microstructure and phase transformations of the high-entropy alloy Cr16Mn16Fe16Co16Ni16P20. The alloy was synthesized via arc melting and subjected to three cooling conditions: slow cooling (52 K/s), accelerated cooling after a short electric arc pulse (3018 K/s), and rapid quenching (10⁵–10⁶ K/s) using the melt-spinning method. The microstructures were characterized using X-ray diffraction (XRD), scanning electron microscopy (SEM), transmission electron microscopy (TEM), and Mössbauer spectroscopy. The thermal properties and phase transformations were analyzed using differential scanning calorimetry (DSC) and thermography. Slow cooling produced a complex crystalline microstructure, while accelerated cooling resulted in fewer phases. Rapid cooling yielded an amorphous structure, demonstrating that phosphorus and high mixing entropy enhance glass-forming ability. Phase transformations exhibited significant undercooling under accelerated cooling, with FCC phase crystallization shifting from 1706 K (slow cooling) to 1341 K, and eutectic crystallization from 1206 K to 960 K. These findings provide a foundation for optimizing cooling processes in high-entropy alloys for advanced structural and functional applications. Full article
(This article belongs to the Special Issue Structure and Properties of Crystalline and Amorphous Alloys-Part II)
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Graphical abstract

Graphical abstract
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<p>DSC results for the Cr<sub>16</sub>Mn<sub>16</sub>Fe<sub>16</sub>Co<sub>16</sub>Ni<sub>16</sub>P<sub>20</sub> alloy during heating (red line) and cooling (blue line) at a rate of 20 K/min. The onset and end temperatures of the endothermic and exothermic transitions are marked, along with the corresponding energy values: −10.1 J/g for the range of 1201.7–1228.1 K and −70.53 J/g for 1299.6–1327.2 K during heating, and −9.1 J/g and −48.3 J/g for cooling at 1151.7 K and 1297.2 K, respectively.</p>
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<p>(<b>a</b>) Thermal images of the arc-melted ingot, with the region of interest (ROI) marked in purple. The image at t = 0.000 s shows the ingot immediately after the extinction of the electric arc. Subsequent images depict the cooling process over time. The temperature-time curve for the ROI is shown in (<b>b</b>), indicating key phase transitions: solidification of phase A at T<sub>1</sub> = 1695 K, precipitation of phase C at T<sub>2</sub> = 1623 K, phase E crystallization at T<sub>3</sub> = 1291 K, eutectic crystallization at T<sub>4</sub> = 1206 K, and a solid-state transformation at T<sub>5</sub> = 1067 K. Cooling after arc melting on a copper plate (52 K/s).</p>
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<p>(<b>a</b>) Thermal images of the ingot with the region of interest (ROI) marked in blue, captured during rapid cooling after a short electric pulse. The image at t = 0.000 s shows the moment the arc was extinguished. The temperature-time curve in (<b>b</b>) highlights key thermal events: solidification at T<sub>1</sub> = 1341 K, precipitation at T<sub>2</sub> = 1270 K (magnified in the inset), a plateau at T<sub>3</sub> = 977 K, a local minimum at T<sub>4</sub> = 960 K, and a solid-state transformation at T<sub>5</sub> = 880 K, visible as a small peak. Cooling after short electric pulse (3018 K/s).</p>
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<p>Microstructure of the Cr<sub>16</sub>Mn<sub>16</sub>Fe<sub>16</sub>Co<sub>16</sub>Ni<sub>16</sub>P<sub>20</sub> alloy ingot after arc remelting. SEM image (<b>a</b>) and elemental distribution maps (<b>b</b>) obtained from EDS analysis for elements P, Cr, Fe, Mn, Co, and Ni. The letters on image (<b>a</b>) correspond to phase and microstructural components described in <a href="#materials-17-05772-t001" class="html-table">Table 1</a>. Sample preparation: Metallographic specimens were mechanically polished and etched using a 3% nitric acid solution in ethanol. SEM observations were performed at an accelerating voltage of 20 kV.</p>
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<p>SEM image of the free surface of the ingot after arc remelting and cooling in a pure argon atmosphere. Dendrites of phase “A”, elongated crystals of phase “E”, and small precipitates of a Cr<sub>2</sub>Mn-like phase with a square-based pyramidal morphology are visible. Sample preparation: Metallographic specimens were mechanically polished and etched using a 3% nitric acid solution in ethanol. SEM observations were performed at an accelerating voltage of 20 kV.</p>
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<p>XRD patterns of the Cr<sub>16</sub>Mn<sub>16</sub>Fe<sub>16</sub>Co<sub>16</sub>Ni<sub>16</sub>P<sub>20</sub> alloy in three different processing states: arc-melted ingot (<b>middle</b>), cold-welded surface (<b>top</b>), and melt-spun ribbon (<b>bottom</b>). The diffraction peaks correspond to FCC, tetragonal (I4), and orthorhombic (ORP) phases. The melt-spun ribbon shows a nearly amorphous structure. XRD test conditions: Scans were performed in the 2θ range of 20°–90° with a step size of 0.02°, at a voltage of 40 kV and a current of 30 mA.</p>
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<p>(<b>a</b>) TEM image showing the amorphous microstructure of the Cr<sub>16</sub>Mn<sub>16</sub>Fe<sub>16</sub>Co<sub>16</sub>Ni<sub>16</sub>P<sub>20</sub> alloy ribbon after melt-spinning. (<b>b</b>) Diffraction pattern with rings, indicating a disordered atomic structure. (<b>c</b>) Intensity profile of the diffraction rings, with two peaks identified at wave vector values of k = 1.169 nm<sup>−1</sup> and k = 2.002 nm<sup>−1</sup>, confirming the amorphous nature of the sample.</p>
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<p>Mössbauer spectra for Cr<sub>16</sub>Mn<sub>16</sub>Fe<sub>16</sub>Co<sub>16</sub>Ni<sub>16</sub>P<sub>20</sub> in different processing states: as-cast ingot (<b>top</b>), after short arc pulse (<b>middle</b>), and melt-spun ribbon (<b>bottom</b>). The spectra were fitted with three components corresponding to different local environments around iron atoms, labeled as Fe1, Fe2, and Fe3. The table includes the relative area (A), isomer shift (IS), and quadrupole splitting (QS) for each component.</p>
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9 pages, 608 KiB  
Article
Foot Sole Temperature Correlates with Ankle–Brachial Index, Pulse Wave Velocity, and Arterial Age in Diabetic Patients Without Diagnosis of Peripheral Arterial Disease
by Blanca Estela Ríos-González, Liliana López-Barragán, Ana Miriam Saldaña-Cruz, Sergio Gabriel Gallardo-Moya, Aniel Jessica Leticia Brambila-Tapia, Carlos Eduardo Soto-Ramirez and Elida Berenice Garcia-Calvario
J. Clin. Med. 2024, 13(21), 6383; https://doi.org/10.3390/jcm13216383 - 25 Oct 2024
Viewed by 835
Abstract
Background/Objectives: Some vascular alterations such as peripheral arterial disease (PAD) or arterial stiffness can alter perfusion of the limbs, so we wondered if this is reflected in the temperature of the soles of the feet of diabetic patients who did not have [...] Read more.
Background/Objectives: Some vascular alterations such as peripheral arterial disease (PAD) or arterial stiffness can alter perfusion of the limbs, so we wondered if this is reflected in the temperature of the soles of the feet of diabetic patients who did not have a diagnosis of peripheral arterial disease. Foot sole temperature was correlated with the ankle–brachial index (ABI), carotid—femoral pulse wave velocity (cfPWV), brachial–ankle pulse wave velocity (baPWV), and arterial age. Methods: A total of 175 patients with type 2 diabetes mellitus, without a previous diagnosis of PAD, were recruited. Comorbidities, anthropometry, biochemical analysis results, temperature, ABI, cfPWV, baPWV, and arterial age were recorded. Forty-two temperature records were obtained from the sole of the foot with an FLIR T865 thermal imaging camera. ABI, cfPWV, baPWV, and arterial age were obtained using plethysmographic and oscillometric methods. Statistical analysis was performed with SPSS v.29.0 (correlations and multiple linear regression models). Results: All temperature points analyzed correlated negatively with ABI (p < 0.001) and rho values ranged from −0.168 to −0.210. Likewise, cfPWV, baPWV, and arterial age had similar results, since most temperature records showed low rho values and a negative correlation with these parameters. Four models were developed to explain the variables of interest. Temperature was involved in all of them. The temperature of the first toe was included in the prediction of cfPWV, baPWV, and arterial age. Conclusions: There is an inversely proportional relationship between temperature and ABI, cfPWV, baPWV, and arterial age in diabetic patients without a previous diagnosis of arterial disease. Temperature can be a predictor of these hemodynamic variables. Full article
(This article belongs to the Section Cardiovascular Medicine)
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<p>Areas of the sole of the foot were analyzed with a thermal imaging camera. The white and yellow areas (warm colors) represent higher temperatures, while the purple and blue regions (cold colors) represent areas with lower temperatures. R: right foot; L: left foot; T: temperature; EI1: area T1 (first toe); EI2: area T2 (second toe); EI3: area T3 (third toe); EI4 area T4 (fourth toe); EI5 area T5 (fifth toe); EI6: area T6 (first metatarsal)); EI7: area T7 (third metatarsal); EI8: area T8 (fifth metatarsal); EI9: area T9 (internal arch); EI10: area T10 (external arch); EI11: area T11 (inner heel); EI12: area T12 (central heel); EI13: area T13 (external heel).</p>
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11 pages, 11529 KiB  
Article
Novel Statistical Analysis Schemes for Frequency-Modulated Thermal Wave Imaging for Inspection of Ship Hull Materials
by Ishant Singh, Vanita Arora, Prabhu Babu and Ravibabu Mulaveesala
NDT 2024, 2(4), 445-455; https://doi.org/10.3390/ndt2040027 - 15 Oct 2024
Viewed by 865
Abstract
In the field of thermal non-destructive testing and evaluation (TNDT&E), active thermography gained popularity due to its fast wide-area monitoring and remote inspection capability to assess materials without compromising their future usability. Among the various active thermographic methods, pulse compression-favorable frequency-modulated thermal wave [...] Read more.
In the field of thermal non-destructive testing and evaluation (TNDT&E), active thermography gained popularity due to its fast wide-area monitoring and remote inspection capability to assess materials without compromising their future usability. Among the various active thermographic methods, pulse compression-favorable frequency-modulated thermal wave imaging stands out for its enhanced detectability and depth resolution. In this study, an experimental investigation has been carried out on a hardened steel sample used in the ship building industry with a flat-bottom-hole-simulated defect using the frequency-modulated thermal wave imaging (FMTWI) technique. The defect detection capabilities of FMTWI have been investigated from various statistical post-processing approaches and compared by taking the signal-to-noise ratio (SNR) as a figure of merit. Among various adopted statistical post-processing techniques, pulse compression has been carried out using different methods, namely the offset removal with polynomial curve fitting and principal component analysis (PCA), which is an unsupervised learning approach for data reduction and offset removal with median centering for data standardization. The performance of these techniques was assessed through experimental investigations on hardened steel specimens used in ship building to provide valuable insights into their effectiveness in defect detection capabilities. Full article
(This article belongs to the Special Issue Advances in Imaging-Based NDT Methods)
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<p>Flow diagram for cross-correlation-based pulse compression with mean removal and PCA.</p>
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<p>Schematic for hardened steel sample with flat bottom hole at center.</p>
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<p>Illustration of the experimental setup used for FMTWI.</p>
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<p>Illustrated (<b>a</b>) raw temporal response and (<b>b</b>) offset-removed profile for FMTWI from 0.01 Hz to 0.1 Hz.</p>
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<p>Reconstructed pulse-compressed (<b>a</b>) spatial thermal distribution and (<b>b</b>) correlation coefficients of offset-removed temporal response for healthy and defective location.</p>
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<p>Reconstructed (<b>a</b>,<b>b</b>) spatial thermal distribution and (<b>c</b>,<b>d</b>) temporal response obtained from PC1 for mean and median centering, respectively.</p>
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<p>Reconstructed (<b>a</b>,<b>b</b>) spatial thermal distribution and (<b>c</b>,<b>d</b>) temporal response obtained from PC2 for mean and median centering, respectively.</p>
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<p>Reconstructed (<b>a</b>,<b>b</b>) spatial thermal distribution and (<b>c</b>,<b>d</b>) temporal response obtained from PC2 for mean and median centering, respectively.</p>
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<p>Reconstructed (<b>a</b>,<b>b</b>) spatial thermal distribution and (<b>c</b>,<b>d</b>) temporal response obtained from PC3 for mean and median centering, respectively.</p>
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<p>Cross-correlation profile for (<b>a</b>) mean-centered and (<b>b</b>) median-centered PC2 thermal profile.</p>
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<p>Illustrated reconstructed spatial thermal distribution obtained by pulse compression of (<b>a</b>) mean-centered and (<b>b</b>) median-centered PC2 signal.</p>
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18 pages, 10325 KiB  
Article
Research on the Detection of Steel Plate Defects Based on SimAM and Twin-NMF Transfer
by Yongqiang Zou, Guanghui Zhang and Yugang Fan
Mathematics 2024, 12(17), 2782; https://doi.org/10.3390/math12172782 - 8 Sep 2024
Cited by 1 | Viewed by 1219
Abstract
Pulsed eddy current thermography can detect surface or subsurface defects in steel, but in the process of combining deep learning, it is expensive and inefficient to build a complete sample of defects due to the complexity of the actual industrial environment. Consequently, this [...] Read more.
Pulsed eddy current thermography can detect surface or subsurface defects in steel, but in the process of combining deep learning, it is expensive and inefficient to build a complete sample of defects due to the complexity of the actual industrial environment. Consequently, this study proposes a transfer learning method based on Twin-NMF and combines it with the SimAM attention mechanism to enhance the detection accuracy of the target domain task. First, to address the domain differences between the target domain task and the source domain samples, this study introduces a Twin-NMF transfer method. This approach reconstructs the feature space of both the source and target domains using twin non-negative matrix factorization and employs cosine similarity to measure the correlation between the features of these two domains. Secondly, this study integrates a parameter-free SimAM into the neck of the YOLOv8 model to enhance its capabilities in extracting and classifying steel surface defects, as well as to alleviate the precision collapse phenomenon associated with multi-scale defect recognition. The experimental results show that the proposed Twin-NMF model with SimAM improves the detection accuracy of steel surface defects. Taking NEU-DET and GC10-DET as source domains, respectively, in the ECTI dataset, [email protected] reaches 99.3% and 99.2%, and the detection accuracy reaches 98% and 98.5%. Full article
(This article belongs to the Section E2: Control Theory and Mechanics)
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Figure 1
<p>Flowchart of Twin-NMF transfer combined with SimAM-YOLOv8.</p>
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<p>The network structure of the Twin-NMF model.</p>
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<p>SimAM-YOLOv8 model network structure.</p>
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<p>Partial NEU-DET, GC10-DET, and ECTI defect images.</p>
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<p>Loss and precision curves of the six groups of experiments.</p>
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<p>Distribution of TNMF selecting samples in source domains.</p>
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<p>3D distribution of source and target domain data under the TNMF.</p>
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13 pages, 3715 KiB  
Article
Thermal Reading of Texts Buried in Historical Bookbindings
by Stefano Paoloni, Giovanni Caruso, Noemi Orazi, Ugo Zammit and Fulvio Mercuri
Sensors 2024, 24(17), 5493; https://doi.org/10.3390/s24175493 - 24 Aug 2024
Viewed by 658
Abstract
In the manufacture of ancient books, it was quite common to insert written scraps belonging to earlier library material into bookbindings. For scholars like codicologists and paleographers, it is extremely important to have the possibility of reading the text lying on such scraps [...] Read more.
In the manufacture of ancient books, it was quite common to insert written scraps belonging to earlier library material into bookbindings. For scholars like codicologists and paleographers, it is extremely important to have the possibility of reading the text lying on such scraps without dismantling the book. In this regard, in this paper, we report on the detection of these texts by means of infrared (IR) pulsed thermography (PT), which, in recent years, has been specifically proven to be an effective tool for the investigation of Cultural Heritage. In particular, we present a quantitative analysis based, for the first time, on PT images obtained from books of historical relevance preserved at the Biblioteca Angelica in Rome. The analysis has been carried out by means of a theoretical model for the PT signal, which makes use of two image parameters, namely, the distortion and the contrast, related to the IR readability of the buried texts. As shown in this paper, the good agreement between the experimental data obtained in the historical books and the theoretical analysis proved that the capability of the adopted PT method could be fruitfully applied, in real case studies, to the detection of buried texts and to the quantitative characterization of the parameters affecting their thermal readability. Full article
(This article belongs to the Section Remote Sensors)
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<p>A book printed in 1758 (ʘ.2.16) from the Biblioteca Angelica of Rome: (<b>a</b>) a picture of the back endleaf; (<b>b</b>) a thermogram recorded 0.02 s after the light pulse, showing the text buried at a depth of 95 μm; (<b>c</b>) a thermogram recorded 0.30 s after the light pulse, also showing the text buried at a depth of 155 μm.</p>
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<p>A book printed in 1592 (f.9.31) from the Biblioteca Angelica of Rome: (<b>a</b>) a picture of the back endleaf; thermograms of the black framed part (area III) recorded 0.02 s (<b>b</b>), 0.05 s (<b>c</b>) and 0.30 s (<b>d</b>) after the light pulse, showing the text buried at a depth of 110 μm.</p>
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<p>A sketch of the specimen considered in the model.</p>
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<p>A sketch of the PT signal profiles over the edge at <math display="inline"><semantics> <mrow> <mover accent="true"> <mrow> <mi>x</mi> </mrow> <mo>¯</mo> </mover> </mrow> </semantics></math> = 0 of a subsurface ink feature, where 1D (black dotted line) and 3D (continuous gray line) heat diffusion regimes are considered. Also represented is the distortion index ∆ (see text).</p>
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<p>The theoretical delay-time dependence of the contrast <span class="html-italic">C</span>(<span class="html-italic">t</span>) (<b>a</b>) and the distortion index ∆(<span class="html-italic">t</span>) (<b>b</b>) over the edge of graphical features buried at different depths in a paper layer.</p>
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<p>Sketches of the bookbinding cross-sections of (<b>a</b>) book ʘ.2.16 and (<b>b</b>) book f.9.31.</p>
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<p>Thermograms of text I buried just beneath the endpaper in the area framed in blue previously shown in <a href="#sensors-24-05493-f001" class="html-fig">Figure 1</a>b, obtained for increasing delay times of 0.02 s (<b>a</b>), 0.05 s (<b>b</b>) and 0.30 s (<b>c</b>) after the heating light pulse. (<b>d</b>) The PT signal profiles obtained over one of the letters.</p>
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<p>Thermograms of text II buried just beneath the endpaper in the area framed in red (previously shown in <a href="#sensors-24-05493-f001" class="html-fig">Figure 1</a>c) obtained for increasing delay times of 0.02 s (<b>a</b>), 0.05 s (<b>b</b>) and 0.30 s (<b>c</b>) after the heating light pulse. (<b>d</b>) The PT signal profiles obtained over one of the letters.</p>
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<p>Thermograms of text III buried just beneath the area framed in black of the endpaper previously shown in <a href="#sensors-24-05493-f002" class="html-fig">Figure 2</a>a, obtained for increasing delay times of 0.02 s (<b>a</b>), 0.05 s (<b>b</b>) and 0.30 s (<b>c</b>) after the heating light pulse. (<b>d</b>) The PT signal profiles obtained over one of the letters.</p>
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<p>The time dependence of (<b>a</b>) the contrast <span class="html-italic">C</span>(<span class="html-italic">t</span>) and (<b>b</b>) distortion ∆ of the texts buried at different depths. The continuous lines represent the theoretical prediction, while the symbols correspond to the experimental data obtained according to the procedure described in the text.</p>
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17 pages, 9478 KiB  
Article
Characterization of Multi-Layer Rolling Contact Fatigue Defects in Railway Rails Using Sweeping Eddy Current Pulse Thermal-Tomography
by Hengbo Zhang, Shudi Zhang, Xiaotian Chen, Yingying Li, Yiling Zou and Yizhao Zeng
Appl. Sci. 2024, 14(16), 7269; https://doi.org/10.3390/app14167269 - 19 Aug 2024
Viewed by 1056
Abstract
Railways play a pivotal role in national economic development, freight transportation, national defense, and regional connectivity. The detection of rolling contact fatigue (RCF) defects in rail tracks is essential for railway safety and maintenance. Due to its efficiency and non-contact capability in detecting [...] Read more.
Railways play a pivotal role in national economic development, freight transportation, national defense, and regional connectivity. The detection of rolling contact fatigue (RCF) defects in rail tracks is essential for railway safety and maintenance. Due to its efficiency and non-contact capability in detecting surface and near-surface defects, Eddy Current Pulsed Thermography (ECPT) has garnered significant attention from researchers. However, detecting multi-layer RCF defects remains a challenge. This paper introduces a sweeping Eddy Current Pulsed Thermal-Tomography system (ECPTT) to detect multi-layer RCF defects effectively. This system utilizes varying excitation frequencies to heat defects, altering skin depth and facilitating feature extraction to distinguish multi-layer RCF defects. Skewness and thermographic signal reconstruction (TSR) values are employed as features in the experiments. These features are qualitatively analyzed to differentiate the layers and depths of multi-layer RCF defects. Additionally, five different coils were compared and analyzed quantitatively. The results indicate that the ECPTT system can effectively detect and distinguish multi-layer RCF defects, thereby providing more detailed defect information and enhancing railway safety and maintenance efficiency. Full article
(This article belongs to the Special Issue Advanced Sensing Technology for Structural Health Monitoring)
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<p>ECPTT schematic diagram.</p>
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<p>Schematic diagram of skinning depth versus frequency.</p>
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<p>Experimental device.</p>
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<p>Excitation coils.</p>
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<p>Excitation coil settings.</p>
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<p>The schema of test piece.</p>
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<p>Skewness of heating results with five coils (the bluer the colour, the greater the negative skewness of the region).</p>
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<p>The attention area of defect.</p>
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<p>Position and skewness of the feature area.</p>
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<p>Temperature variation diagram of defects with different depths.</p>
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<p>Temperature variation diagram of defects with different layers.</p>
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23 pages, 9322 KiB  
Article
Defect Detection of GFRP Composites through Long Pulse Thermography Using an Uncooled Microbolometer Infrared Camera
by Murniwati Anwar, Faizal Mustapha, Mohd Na’im Abdullah, Mazli Mustapha, Nabihah Sallih, Azlan Ahmad and Siti Zubaidah Mat Daud
Sensors 2024, 24(16), 5225; https://doi.org/10.3390/s24165225 - 12 Aug 2024
Viewed by 1091
Abstract
The detection of impact and depth defects in Glass Fiber Reinforced Polymer (GFRP) composites has been extensively studied to develop effective, reliable, and cost-efficient assessment methods through various Non-Destructive Testing (NDT) techniques. Challenges in detecting these defects arise from varying responses based on [...] Read more.
The detection of impact and depth defects in Glass Fiber Reinforced Polymer (GFRP) composites has been extensively studied to develop effective, reliable, and cost-efficient assessment methods through various Non-Destructive Testing (NDT) techniques. Challenges in detecting these defects arise from varying responses based on the geometrical shape, thickness, and defect types. Long Pulse Thermography (LPT), utilizing an uncooled microbolometer and a low-resolution infrared (IR) camera, presents a promising solution for detecting both depth and impact defects in GFRP materials with a single setup and minimal tools at an economical cost. Despite its potential, the application of LPT has been limited due to susceptibility to noise from environmental radiation and reflections, leading to blurry images. This study focuses on optimizing LPT parameters to achieve accurate defect detection. Specifically, we investigated 11 flat-bottom hole (FBH) depth defects and impact defects ranging from 8 J to 15 J in GFRP materials. The key parameters examined include the environmental temperature, background reflection, background color reflection, and surface emissivity. Additionally, we employed image processing techniques to classify composite defects and automatically highlight defective areas. The Tanimoto Criterion (TC) was used to evaluate the accuracy of LPT both for raw images and post-processed images. The results demonstrate that through parameter optimization, the depth defects in GFRP materials were successfully detected. The TC success rate reached 0.91 for detecting FBH depth defects in raw images, which improved significantly after post-processing using Canny edge detection and Hough circle detection algorithms. This study underscores the potential of optimized LPT as a cost-effective and reliable method for detecting defects in GFRP composites. Full article
(This article belongs to the Section Sensor Materials)
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Graphical abstract

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<p>Radiation captured during data measurement using an IR camera [<a href="#B33-sensors-24-05225" class="html-bibr">33</a>].</p>
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<p>Front rear of the eleven flat bottom holes (FBH) of the GFRP sample.</p>
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<p>Impact defect of the GFRP sample: (<b>a</b>) sample IM1 and (<b>b</b>) sample IM2.</p>
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<p>LPT setup using (<b>a</b>) reflex configurations and (<b>b</b>) an enclosure.</p>
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<p>Example of black-colored paper used in the experiment.</p>
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<p>Close setup of the enclosure using hard cardboard.</p>
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<p>Surface material covered with color tape.</p>
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<p>Image-segmentation method for automatic defect detection.</p>
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<p>Edge detection flowchart.</p>
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<p>Circle detection algorithm flowchart.</p>
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<p>Outdoor output image at temperatures above 35 °C for 10–40 s of heating duration.</p>
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<p>Indoor output image at room temperature (23–25 °C) for 10–40 s of heating duration.</p>
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<p>Indoor output image at low temperatures (16–18 °C) for 10–40 s of heating duration.</p>
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<p>Temperature bar for one of the images captured outdoors at temperatures above 35 °C.</p>
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<p>Output image for the black-colored background of the internal wall for 20–40 s of heating.</p>
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<p>Output image for the white-colored background of the internal wall for 20–40 s of heating.</p>
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<p>Output image for the yellow-colored background of the internal wall for 20–40 s of heating.</p>
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<p>Result for indoors, without an enclosure at temperatures from 16 °C to 18 °C from 20 s (first row) to 40 s (last row) of heating.</p>
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<p>Result for indoors, using an enclosure at temperatures from 16 °C to 18 °C from 20 s (first row) to 40 s (last row) of heating.</p>
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<p>Without tape covered on the surface material at low temperatures (16° C to 18 °C) from 10 s (first row) to 40 s (last row) of heating.</p>
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<p>Yellow tape covered on top of the surface sample at low temperatures (16 °C to 18 °C) from 10 s (first row) to 40 s (last row) of heating.</p>
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<p>With black tape on the surface material at low temperatures (16 °C to 18 °C) from 10 s (first row) to 40 s (last row) of heating.</p>
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<p>Optimized FBH defect of the GFRP detected.</p>
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<p>Impact defect detection results using optimized parameters for samples (<b>a</b>) B1 and (<b>b</b>) B2.</p>
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<p>FBH depth defect detection process using Canny edge detection segmentation.</p>
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<p>FBH depth defect detection process using Sobel edge detection segmentation.</p>
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<p>Edge image segmentation for GFRP impact defect detection using the Canny edge detection method for (<b>a</b>) defect IM1 and (<b>b</b>) defect IM2.</p>
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<p>FBH depth defect detection using histogram threshold.</p>
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<p>Histogram threshold segmentation method result for (<b>a</b>) defect IM1 and (<b>b</b>) defect IM2.</p>
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<p>FBH defect detection using the circle segmentation method.</p>
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35 pages, 2501 KiB  
Review
Thermal Material Property Evaluation Using through Transmission Thermography: A Systematic Review of the Current State-of-the-Art
by Zain Ali, Sri Addepalli and Yifan Zhao
Appl. Sci. 2024, 14(15), 6791; https://doi.org/10.3390/app14156791 - 3 Aug 2024
Viewed by 1192
Abstract
Determining thermal material properties such as thermal diffusivity can provide valuable insights into a material’s thermal characteristics. A well-established method for this purpose is flash thermography using Parker’s half-rise equation. It assumes one-dimensional heat transfer for thermal diffusivity estimation through the thickness of [...] Read more.
Determining thermal material properties such as thermal diffusivity can provide valuable insights into a material’s thermal characteristics. A well-established method for this purpose is flash thermography using Parker’s half-rise equation. It assumes one-dimensional heat transfer for thermal diffusivity estimation through the thickness of the material. However, research evidence suggests that the technique has not developed as much as the reflection mode over the last decade. This systematic review explores the current state-of-the-art in through-transmission thermography. The methodology adopted for this review is the SALSA framework that seeks to Search, Appraise, Synthesise, and Analyse a selected list of papers. It covers the fundamental physics behind the technique, the advantages/limitations it has, and the current state-of-the-art. Additionally, based on the Population, Intervention, Comparison, Outcome, and Context (PICOC) framework, a specific set of inclusion and exclusion criteria was determined. This resulted in a final list of 81 journal/conference papers selected for this study. These papers were analysed both quantitatively and quantitatively to identify and address the current knowledge gap hindering the further development of through-transmission thermography. The findings from the review outline the current knowledge gap in through-transmission thermography and the challenges hindering the development of the technique, such as depth quantification in pulsed thermography and the lack of a standardised procedure for conducting measurements in the transmission mode. Overcoming some of these obstacles can pave the way for further development of this method to aid in material characterisation. Full article
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<p>The various NDT methods.</p>
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<p>Schematic of 1D heat transfer on a semi-infinite plate with heat flowing in the z-direction.</p>
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<p>Names of authors with two or more publications.</p>
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<p>Common keywords (occurring at least 2 or more times).</p>
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<p>Distribution of papers published in journals and conferences.</p>
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<p>Number of publications per year.</p>
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<p>(<b>a</b>) The reflection and (<b>b</b>) transmission configurations with their respective temperature profiles (graphs have been generated using MATLAB R2023a).</p>
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<p>(<b>a</b>) Schematic for pulsed thermography using COMSOL v.6.0 with the temperature response of the defect and defect-free areas for an 8 mm radius defect at 1 mm depth (as viewed from the front wall) at the (<b>b</b>) front wall (<b>c</b>) back wall. Plots have been generated using Microsoft Excel v.2406.</p>
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18 pages, 6204 KiB  
Article
A Complementary Fusion-Based Multimodal Non-Destructive Testing and Evaluation Using Phased-Array Ultrasonic and Pulsed Thermography on a Composite Structure
by Muhammet E. Torbali, Argyrios Zolotas, Nicolas P. Avdelidis, Muflih Alhammad, Clemente Ibarra-Castanedo and Xavier P. Maldague
Materials 2024, 17(14), 3435; https://doi.org/10.3390/ma17143435 - 11 Jul 2024
Cited by 1 | Viewed by 1000
Abstract
Combinative methodologies have the potential to address the drawbacks of unimodal non-destructive testing and evaluation (NDT & E) when inspecting multilayer structures. The aim of this study is to investigate the integration of information gathered via phased-array ultrasonic testing (PAUT) and pulsed thermography [...] Read more.
Combinative methodologies have the potential to address the drawbacks of unimodal non-destructive testing and evaluation (NDT & E) when inspecting multilayer structures. The aim of this study is to investigate the integration of information gathered via phased-array ultrasonic testing (PAUT) and pulsed thermography (PT), addressing the challenges posed by surface-level anomalies in PAUT and the limited deep penetration in PT. A center-of-mass-based registration method was proposed to align shapeless inspection results in consecutive insertions. Subsequently, the aligned inspection images were merged using complementary techniques, including maximum, weighted-averaging, depth-driven combination (DDC), and wavelet decomposition. The results indicated that although individual inspections may have lower mean absolute error (MAE) ratings than fused images, the use of complementary fusion improved defect identification in the total number of detections across numerous layers of the structure. Detection errors are analyzed, and a tendency to overestimate defect sizes is revealed with individual inspection methods. This study concludes that complementary fusion provides a more comprehensive understanding of overall defect detection throughout the thickness, highlighting the importance of leveraging multiple modalities for improved inspection outcomes in structural analysis. Full article
(This article belongs to the Special Issue Structural Health Monitoring of Polymer Composites)
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<p>Specimen specifications.</p>
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<p>NDT &amp; E experimental setup and representative demonstration of base signals for PAUT. (<b>a</b>) PAUT transducer and equipment setup for inspection; (<b>b</b>) a symbolic PAUT frame of signals including defective peaks and sound region through the thickness.</p>
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<p>NDT &amp; E setup for PT and a representative demonstration of PT lines. (<b>a</b>) PT setup in reflection mode; (<b>b</b>) arbitrary line profiles showing heat differences on defective and sound parts.</p>
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<p>Canny edge detection performance criteria demonstrations of an example defected PT line profile. (<b>a</b>) Representative noisy line from a PT image; (<b>b</b>) stronger responses at edge positions in the smoothed line; (<b>c</b>) good localization with local maximums in a reasonable neighborhood.</p>
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<p>Representative registered image pair based on center-of-mass matching. (<b>a</b>) Fixed PAUT image as a reference for required transformation. (<b>b</b>) Registered PT image, which has a slight rotation.</p>
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<p>PAUT inspection results for delamination lines with different thicknesses. (<b>a</b>) PAUT inspection result for Line 1: 1 mm thickness; (<b>b</b>) PAUT inspection result for Line 2: 0.6 mm thickness; (<b>c</b>) PAUT inspection result for Line 3: 0.2 mm thickness; (<b>d</b>) PAUT inspection result for Line 4: 0.4 mm thickness; (<b>e</b>) PAUT inspection result for Line 5: 0.8 mm thickness.</p>
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<p>PT inspe ction results for delamination lines with different thicknesses. (<b>a</b>) PT inspection result for Line 1: 1 mm thickness; (<b>b</b>) PT inspection result for Line 2: 0.6 mm thickness; (<b>c</b>) PT inspection result for Line 3: 0.2 mm thickness; (<b>d</b>) PT inspection result for Line 4: 0.4 mm thickness; (<b>e</b>) PT inspection result for Line 5: 0.8 mm thickness.</p>
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<p>PA and PT inspections’ binary images for delamination lines with different thicknesses. (<b>a</b>) PA binary image for Line 1: 1 mm thickness; (<b>b</b>) PT binary image for Line 1: 1 mm thickness; (<b>c</b>) PA binary image for Line 2: 0.6 mm thickness; (<b>d</b>) PT binary image for Line 2: 0.6 mm thickness; (<b>e</b>) PA binary image for Line 3: 0.2 mm thickness; (<b>f</b>) PT binary image for Line 3: 0.2 mm thickness; (<b>g</b>) PA binary image for Line 4: 0.4 mm thickness; (<b>h</b>) PT binary image for Line 4: 0.4 mm thickness; (<b>i</b>) PA binary image for Line 5: 0.8 mm thickness; (<b>j</b>) PT binary image for Line 5: 0.8 mm thickness.</p>
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<p>Fusion images with different combination rules for overall detection. (<b>a</b>) Maximum fusion rule detection images; (<b>b</b>) weighted-average rule detection images; (<b>c</b>) DDC rule detection images; (<b>d</b>) wavelet decomposition fusion detection images.</p>
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16 pages, 8162 KiB  
Article
Wear Characterization of Cold-Sprayed HEA Coatings by Means of Active–Passive Thermography and Tribometer
by Raffaella Sesana, Luca Corsaro, Nazanin Sheibanian, Sedat Özbilen and Rocco Lupoi
Lubricants 2024, 12(6), 222; https://doi.org/10.3390/lubricants12060222 - 17 Jun 2024
Cited by 1 | Viewed by 933
Abstract
The aim of this work is to verify the applicability of thermography as a non-destructive technique to quantify the wear performance of several high-entropy alloy coatings. Thermal profiles obtained from passive and active thermography were analyzed and the results were correlated with the [...] Read more.
The aim of this work is to verify the applicability of thermography as a non-destructive technique to quantify the wear performance of several high-entropy alloy coatings. Thermal profiles obtained from passive and active thermography were analyzed and the results were correlated with the classical tribological approaches defined in standards. HEA coatings made of several chemical compositions (AlxCoCrCuFeNi and MnCoCrCuFeNi) and realized by using different cold spray temperatures (650 °C, 750 °C, and 850 °C) were tested in a pin-on-disk configuration, with a dedicated pin developed for the wear tests. Then, the wear performances of each sample were analyzed with the hardness and wear parameter results. The thermal profiles of passive and active thermography allowed a complete characterization of the wear resistance and performance analysis of the coatings analyzed. The results are also compared with those presented in the literature. Full article
(This article belongs to the Special Issue Wear-Resistant Coatings and Film Materials)
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<p>Tested samples (<b>left</b> side) and geometrical shape (<b>right</b> side).</p>
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<p>Designed pin and experimental setup during wear tests.</p>
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<p>Area (<b>left side</b>) and 3D optical microscope comparison (<b>right side</b>) for Sample 5.</p>
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<p>Passive thermography experimental setup.</p>
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<p>Active thermography equipment and experimental setup.</p>
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<p>Normalized relative radiance profiles for samples 2 and 7.</p>
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<p>Measured Δ<span class="html-italic">Volume</span> (column) and Δ<span class="html-italic">Area</span> (line) (<b>a</b>) and abraded mass (<b>b</b>) for different samples.</p>
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<p>Wear rate (column) and Archard’s coefficient (line) (<b>a</b>); wear resistance vs. hardness (<b>b</b>).</p>
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<p>SEM images for samples 1 and 2.</p>
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<p>SEM images for 100Cr6 disks.</p>
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<p>Coefficients of friction and temperature profiles.</p>
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<p>Coefficients of friction (mean value) and maximum temperature increments.</p>
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<p>Δ<span class="html-italic">Volume</span> (orange) and abraded mass (green) vs. <math display="inline"><semantics> <mrow> <mo>Δ</mo> <msub> <mi>A</mi> <mrow> <mi>T</mi> <mi>h</mi> <mi>e</mi> <mi>r</mi> <mi>m</mi> <mi>a</mi> <mi>l</mi> </mrow> </msub> </mrow> </semantics></math></p>
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<p>Δ<span class="html-italic">Volume</span> (<b>a</b>) and abraded mass (<b>b</b>) vs. <math display="inline"><semantics> <mrow> <mo>Δ</mo> <msub> <mi>A</mi> <mrow> <mi>C</mi> <mi>o</mi> <mi>o</mi> <mi>l</mi> <mi>i</mi> <mi>n</mi> <mi>g</mi> </mrow> </msub> </mrow> </semantics></math></p>
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5 pages, 1149 KiB  
Proceeding Paper
Spatial Structure Analysis for Subsurface Defect Detection in Materials Using Active Infrared Thermography and Adaptive Fixed-Rank Kriging
by Chun-Han Chang, Stefano Sfarra, Nan-Jung Hsu and Yuan Yao
Eng. Proc. 2023, 51(1), 43; https://doi.org/10.3390/engproc2023051043 - 14 Dec 2023
Viewed by 619
Abstract
The study focuses on reducing noise and nonstationary backgrounds in data collected through active infrared thermography (AIRT) for defect detection in materials. The authors employ adaptive fixed-rank kriging to analyze a sequence of thermograms obtained in the AIRT experiment. Using basis functions derived [...] Read more.
The study focuses on reducing noise and nonstationary backgrounds in data collected through active infrared thermography (AIRT) for defect detection in materials. The authors employ adaptive fixed-rank kriging to analyze a sequence of thermograms obtained in the AIRT experiment. Using basis functions derived from thin-plate splines, the data features are represented at various resolution levels, resulting in a concise spatial covariance function representation. Eigenfunctions are then derived from the estimated covariance function to capture spatial structures at different scales. Visualizing these eigenfunctions highlights defect information. The authors validate their approach through a pulsed thermography experiment on a carbon-fiber-reinforced plastic (CFRP) sample, demonstrating its effectiveness in detecting defects. Full article
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<p>The first 10 frames of thermograms collected in the experiment.</p>
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<p>The first two eigenfunctions derived from autoFRK.</p>
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13 pages, 5710 KiB  
Article
A Dataset of Pulsed Thermography for Automated Defect Depth Estimation
by Ziang Wei, Ahmad Osman, Bernd Valeske and Xavier Maldague
Appl. Sci. 2023, 13(24), 13093; https://doi.org/10.3390/app132413093 - 8 Dec 2023
Cited by 1 | Viewed by 1644
Abstract
Pulsed thermography is an established nondestructive evaluation technology that excels at detecting and characterizing subsurface defects within specimens. A critical challenge in this domain is the accurate estimation of defect depth. In this paper, a new publicly accessible pulsed infrared dataset for PVC [...] Read more.
Pulsed thermography is an established nondestructive evaluation technology that excels at detecting and characterizing subsurface defects within specimens. A critical challenge in this domain is the accurate estimation of defect depth. In this paper, a new publicly accessible pulsed infrared dataset for PVC specimens is introduced. It was enriched with 3D positional information to advance research in this area. To ensure the labeling quality, a comparative analysis of two distinct data labeling methods was conducted. The first method is based on human domain expertise, while the second method relies on 3D CAD images. The analysis showed that the CAD-based labeling method noticeably enhanced the precision of defect dimension quantification. Additionally, a sophisticated deep learning model was employed on the data, which were preprocessed by different methods to predict both the two-dimensional coordinates and the depth of the identified defects. Full article
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<p>CAD image for all the possible defects’ locations, sizes, and depths.</p>
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<p>Experiment set up of PT inspection.</p>
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<p>Comparison of original infrared frame and resulting images generated by TSR, PPT, and PCT, respectively.</p>
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<p>PCT images and labeled images, where different grayscale values represent different depths.</p>
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<p>PCT images (<b>top</b>) generated from 3D files and the depth images (<b>bottom</b>).</p>
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<p>Comparison of mask images labeled by the manual method and the 3D-CAD-based approach, where the green masks are labeled by the manual method and the red masks are labeled by the 3D CAD-based method. Yellow areas highlight the overlap between these two masks.</p>
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<p>Reference distance from point A to point B. The left image shows this distance on the CAD image. The right image illustrates the corresponding distance on the PCT image.</p>
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<p>Network architecture of YOLOv5 model from [<a href="#B34-applsci-13-13093" class="html-bibr">34</a>], which is licensed under CC BY 4.0.</p>
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<p>Comparison of training images generated by TSR, PPT, and PCT, respectively.</p>
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<p>Confusion matrix of the results on the datasets preprocessed through TSR, PPT, and PCT.</p>
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5 pages, 30149 KiB  
Proceeding Paper
Train Pulses with a Random Spatial Distribution to Measure In-Plane Thermal Diffusivity
by Paolo Bison, Giovanni Ferrarini, Christ Glorieux, Shuji Kamegaki, Junko Morikawa, Stefano Rossi and Meguya Ryu
Eng. Proc. 2023, 51(1), 39; https://doi.org/10.3390/engproc2023051039 - 30 Nov 2023
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Abstract
A thermal diffusivity measurement approach is proposed in which the sample is thermally excited by a periodic train of pulsed, spatially random laser light. The temperature field on the surface is observed by IR camera and the diffusion is recorded by a sequence [...] Read more.
A thermal diffusivity measurement approach is proposed in which the sample is thermally excited by a periodic train of pulsed, spatially random laser light. The temperature field on the surface is observed by IR camera and the diffusion is recorded by a sequence of IR images. The analysis of the diffusion in time and space is followed by suitable models. Fitting of the spatiotemporal evolution of the surface temperature allows to determine the thermal diffusivity of clay brick with an accuracy of 5%. Full article
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Figure 1

Figure 1
<p>The semi-infinite body with no heat exchange with the environment, and prescribed heating function <math display="inline"><semantics> <mrow> <mi>f</mi> <mo>(</mo> <mi>x</mi> <mo>,</mo> <mi>y</mi> <mo>)</mo> </mrow> </semantics></math> on the surface and Dirac delta <math display="inline"><semantics> <mrow> <mi>δ</mi> <mo>(</mo> <mi>t</mi> <mo>)</mo> </mrow> </semantics></math> in time.</p>
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<p>(<b>a</b>) Clay brick sample; (<b>b</b>) sample mounted in holder; (<b>c</b>) random pattern mounted in front of the exit of the laser; (<b>d</b>) experimental layout: the yellow dashed line indicates the field of view of the IR camera, the green arrow indicates the incident laser beam.</p>
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<p>Eight random patterns were prepared in the facilities of the <span class="html-italic">Tokyo Tech</span> and <span class="html-italic">Tsukuba AIST</span>. A 100 nm layer of gold was sputtered on a glass substrate.</p>
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<p>IR image immediately after the shot of the laser. The camera was running in windowing mode with images of 80 × 320 pixels at 150 Hz frame rate.</p>
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<p>Each point in the plot is the slope of the straight line that fits the amplitude of the spatial Fourier Transform of the IR image at a certain spatial frequency. The slopes depend quadratically on the spatial frequency <span class="html-italic">k</span> and the coefficient of the quadratic term in the parabola is the thermal diffusivity.</p>
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