新页面
Non-destructiveInvestigation Testingon the corrosion resistance of Insulatingepoxy Materialsresin Defectscoatings Basedmodified onby Terahertzhigh-entropy Time-domainoxides
Spectroscopy System
Xiaoyu Luoa,BoxinYanb,Yan1, ChaoWangb,*Wang1,2,MingYihuiNieaLiu1Hubei
a1HubeiElectricKeyPower Research InstituteLaboratory ofGuangdongAdvancedPowerTechnologyGridforCo.,Ltd.AutomotiveGuangzhouComponents510080,&China
bCollaborative Innovation Center for Automotive Components Technology, Wuhan University of Technology,WuhanWuhan, Hubei, 430070,Hubei,China
Abstract2Corresponding-author’sInsulatinge-mail:materialswchao@whut.edu.cnareAbstract:
widelyHigh-entropyused in fields suchoxides, aspowerangrids,emergingelectricalclassengineering,of ceramic materials, exhibit exceptional high-temperature stability, superior corrosion resistance, andautomotiveexcellentmanufacturing.hardnessHowever,anddefectsstrength,suchrendering them promising candidates for surface protection applications. In this study, high-entropy oxide filler Y2(Ti0.2Zr0.2Hf0.2Ce0.2V0.2)2O7 was synthesized via solid-state reaction and incorporated asbubblesa nanofiller to modify epoxy resin, thereby fabricating composite coatings. The influence of varying high-entropy oxide contents on the anticorrosion performance of the composite coatings was systematically investigated, andinclusionstheoftenunderlyingarisecorrosionduringprotectiontheirmechanismprocessing and service, which not only affect performance but may also pose potential safety hazards. Terahertz technology, with its low radiation and high penetration characteristics, has become a new method forof thenon-destructivehigh-entropytesting of insulating materials. However, its imaging is limited by hardware and optical diffraction constraints, leading to issues such as low resolution, high noise, and low contrast. This study focuses onoxide-modified epoxyresincoatingsinsulatingwasmaterialselucidated.and employs a reflective terahertz time-domain spectroscopy system to perform point-by-point sampling, obtaining waveforms and images for detecting internal defects such as bubbles and inclusions, and analyzing the differences in defect characteristics. To address the issue of inadequate image quality, a preprocessing method combining non-local means filtering and contrast-limited adaptive histogram equalization is proposed to suppress noise and enhance local contrast. Additionally, the SRCNN network is applied for super-resolution reconstruction to improve image details and resolution. ExperimentalThe results demonstrate that theproposedcompositemethodcoatingseffectivelyincorporatingalleviateshigh-entropyissuesoxidesuchexhibit outstanding anticorrosion properties, with a corrosion inhibition efficiency of 99.39% derived from polarization curve analysis. Even after immersion in 3.5wt% NaCl solution for 10 days, the corrosion inhibition efficiency remained at 95.57%. Impedance efficiency, aslowdeterminedresolutionfrom Nyquist plots, reached 98.63%, andlowretainedcontrast91.75% after 10 days of immersion.
1. Introduction
Metallic materials play a crucial role in terahertzindustrial images,development. significantlyTheir improvingcorrosion defectnot detectiononly accuracyaffects the national economy and reliability.
Keywords:safety, insulatingbut material,also terahertz,poses non-destructivesignificant testing,environmental imageimpacts. enhancement,Among super-resolutionexisting reconstruction
Introduction
applying Insulationprotective materialscoatings serveon asmetal surfaces is currently one of the foundation for the development of electrical products and aremost widely used inand numerouseffective fields,corrosion-prevention approaches [1]. However, traditional organic coatings often fail to meet the demands of modern industry, and the incorporation of functional anticorrosive fillers has proven to be an effective method to enhance coating performance [2].
One-dimensional nanomaterials exhibit size-dependent effects [3] and barrier properties, which can effectively improve the performance of epoxy coatings by mitigating microcracks and voids formed during the curing process [4]. High-entropy oxides represent a novel class of ceramic materials [5], composed of multiple metallic elements that form a highly disordered structure. This unique configuration imparts exceptional properties, including powersuperior grids,thermal electricalstability, engineering,outstanding automobilecorrosion manufacturing,resistance, and aerospace.excellent Forhardness instance,and mechanical strength. In this study, one-dimensional high-entropy oxide nanofillers were synthesized and incorporated into epoxy resin to develop composite coatings. The objective is commonlyto employedfill asmicro-voids a supporting insulation component in high-voltage equipment such as GIL/GIS and cable terminals[1], which can reduce installation time by 80% and maintain partial discharge levels below 5pC. However, internal defects such as bubbles, cracks, impurities, and aging inevitably arisegenerated during the productioncoating fabrication process, thereby achieving a composite coating with enhanced hardness and servicecorrosion liferesistance, and subsequently investigating its anticorrosion performance.
2. Methods and Materials
2.1 Preparation of insulationHigh-Entropy materialOxide components.Y2(Ti0.2Zr0.2Hf0.2Ce0.2V0.2)2O7
The defectshigh-entropy notoxide only(HEO) compromisewas synthesized using the material’ssolid-state normalreaction operationmethod. butThe maymain alsopreparation leadsteps toare functionalas failures,follows: severeoxide accidents, and significant economic losses. In practical engineering, there is a demand to detect potential internal defects in insulation materials without damaging power grid equipment, thereby assessing the extent of degradation. Non-destructive testing of insulation materials not only ensures equipment safety and extends service life but also improves operational efficiency and reduces costs. For example, the cost of timely repair for partial discharge in cable joints is merely 10%-20%powders of the expensecorresponding requiredelements were weighed according to the designed chemical composition of the high-entropy oxide with a molar ratio of Y:T:Zr:Hf:Ce:V = 5:1:1:1:1:1. The powders were then mixed using a planetary ball mill for post-failure12 replacement.hours. After milling, the resulting slurry was transferred into centrifuge tubes, centrifuged, and the lower precipitate was collected and dried in a vacuum oven for 8 hours. The dried mixture was subsequently ground and sieved through a 200-mesh sieve. The sieved powder was placed in an alumina crucible, compacted with a spatula, and sintered in a muffle furnace at 1000 °C for 4 hours. Finally, the sintered product was ground and passed through a 200-mesh sieve to obtain the high-entropy oxide filler (HEO).
2.2 Preparation of Composite Coatings
2g of epoxy resin was dissolved in 8mL of acetone, followed by the addition of 40mg of high-entropy oxide filler and ultrasonic dispersion for 15min. The slurry was then heated and stirred at 50°C to remove the acetone. Subsequently, 0.6g of curing agent T-31 was added, and the mixture was stirred at a constant speed for 15min. The coating was uniformly applied onto the pretreated 6061 aluminum alloy surface using a wire-wound rod coater with a wet film thickness of 200μm. The prepared samples were cured at room temperature for 2 days, followed by heating at 60°C for 4h, yielding an epoxy resin composite coating with a high-entropy oxide incorporation of 2wt%, designated as HEO-2.
Following the same procedure, composite coating samples with filler mass fractions of 1wt% and 3wt% were prepared and designated as HEO-1 and HEO-3, respectively. Additionally, a pure epoxy resin coating without any filler was fabricated and designated as EPa2 + b2 = c2 .
$$\left( x + a \right)^{n} = \sum_{k = 0}^{n}{\left( \frac{n}{k} \right)x^{n - k}a^{k}}$$
The commonmorphological non-destructive testing methods currently used in the power grid field include infrared inspection, ultrasonic testing, and X-ray detection. Infrared inspection can only detect surface or near-surface defects and is highly sensitive to environmental temperature, limiting its effectiveness. Ultrasonic testing faces difficulties when detecting curved components and has poor penetration ability for high attenuation materials. X-ray inspection generates ionizing radiation, posing certain safety risks. Terahertz waves refer to electromagnetic waves with frequencies between 0.1 THz and 10 THz, corresponding to wavelengths ranging from approximately 0.03 to 3 mm. Terahertz waves have good penetration capabilities, easily passing through most non-polar materials and dielectric materials. They are also highly safe, as the energy of terahertz photons is very low compared to X-rays and does not cause damage to the material being tested due to ionizing radiation. Furthermore, terahertz waves have unique fingerprint spectral characteristics, which can be used for the exclusive identification and analysis of materials. Therefore, terahertz non-destructive testing technology is suitable for internal non-destructive inspection of insulating materials.
Terahertz imaging is achieved through point-by-point scanning of a sample. By extracting the time-domain and frequency-domain characteristicsfeatures of the terahertzEP, reflectedHEO-1, waves from the sample, pixel values are assignedHEO-2, and convertedHEO-3 intosamples grayscalewere image data to generate the terahertz image. However, due to limitations such as terahertz wavelength, signal attenuation, noise interference, and hardware constraints of imaging systems, current terahertz images still suffer from issues like low spatial resolution, poor contrast, and blurred contours. To address these challenges, two primary solutions exist: first, enhancing hardware precision to improve terahertz image resolution, and second,observed using ascanning super-resolutionelectron reconstruction [2] algorithm post-processing to refine acquired terahertz images for higher resolution. Notably, the second approach proves more cost-effective. To enhance imaging quality, improve defect recognition accuracy, and precisely characterize internal defects in insulation materials, this paper proposes a preprocessing method combining non-local mean filtering with contrast-limited histogram equalization, alongside an improved SRCNNmicroscopy (Super-Resolution Convolutional Neural Network) for terahertz image super-resolution reconstruction. The effectiveness of this methodology is validated through experimental testing on epoxy resin insulation material defect samples.SEM).
2. Basic principles
2.1 Principle of Terahertz Time Domain Spectroscopy System
The workingelectrochemical principleimpedance spectroscopy (EIS) and polarization curves of the reflectivecoatings terahertzwere time-domainmeasured spectroscopyusing system[3]an iselectrochemical shownworkstation. inEIS Figuremeasurements 1.were Aconducted femtosecondat laseropen-circuit generatespotential laser pulses, which are split into two beams after passing throughover a half-wavefrequency platerange from 100,000Hz to 0.01Hz, with an AC amplitude of 10mV. Polarization curves were recorded at a scan rate of 5mV/s. The corrosion inhibition efficiency [6] and aimpedance polarizer.efficiency The reflected beam serves as the pump light, while the refracted beam is the probe light. The pump light passes through another half-wave plate and polarizer, then is delayed optically before being focused onto a photoconductive antenna to generate terahertz pulses. After being reflected by a set of parabolic mirrors, the terahertz pulses are directed towards the sample under test. The probe light is focused onto the opposite end[7] of the detectioncoated antennasamples afterwere passingcalculated through a mirror and a lens. The probe light generates photo-induced carriers inusing the focalfollowing region of the detector, which are used to detect the instantaneous electric field amplitude of the terahertz pulse, thereby enabling terahertz detection and obtaining the terahertz time-domain waveform.

Figure 1 Schematic diagram of the reflective terahertz time-domain spectroscopy (THz-TDS) system
Figure 2 illustrates a terahertz time-domain spectroscopy scanning imaging system. The epoxy resin sample is placed on a two-dimensional scanning translation stage, with the mainframe and PC turned on, and testing begins after the mainframe has warmed up. The height of the translation stage is adjusted to maximize the peak-to-peak difference of the time-domain signal[4], in order to prevent diffraction effects from adversely affecting the terahertz image. The stepper motor driver, controlled by the PC, drives the stepper motor to move the stage, and a reflected terahertz signal is obtained for each pixel movement. The information from the obtained terahertz signal is used to assign values to the pixels, and these values are then converted into grayscale to produce the sample’s original terahertz image[5]. When defects are present along the optical path of the terahertz wave, the received terahertz wave undergoes distortion due to reflection at the defect interface. In the time domain, this manifests as changes in the pulse peak size, flight time, and signal envelope area, while in the frequency domain, it primarily manifests as variations in the amplitude of frequency components and changes in spectral energy.
Figure 2 Reflective terahertz time-domain spectroscopy (THz-TDS) scanning imaging system
2.2 Principle of Terahertz Image Super-Resolution Reconstruction
The terahertz image super-resolution reconstruction model used in this study consists of two parts: the first part is the preprocessing module, and the second part is the SRCNN network. The first part aims to perform denoising and image enhancement on the original terahertz image, while the second part aims to improve the spatial resolution of the terahertz image. The training network is shown in the figure. The first part mainly implements denoising and contrast enhancement through non-local mean filtering and contrast-limited histogram equalization, while the second part uses the SRCNN network, which consists of feature extraction layers, nonlinear mapping layers, and high-resolution reconstruction layers to achieve resolution enhancement.
Due to the physical characteristics of terahertz waves and the point-by-point scanning imaging method, the resulting terahertz images have pixels that are relatively isolated from each other. This leads to issues such as high noise, low contrast, and blurry edges, requiring preprocessing. This paper primarily employs the non-local mean filtering algorithm to remove background noise and uses contrast-limited histogram equalization to enhance the contrast of the terahertz image.
To address the problem of isolated pixels and unclear textures in the original terahertz images, the non-local mean filtering method[6] is applied for denoising, with the algorithm schematic shown in Figure 3. This algorithm requires calculating the similarity between all pixels and the current pixel. In practice, a large search window and a small neighborhood window are first defined, with the neighborhood window sliding within the search window. The weights are determined based on the similarity between the neighborhoods. The formula for non-local mean filtering is as follows:equations.
| (2) |
Here,In Equation (1), P represents the weight,corrosion indicatinginhibition efficiency, ji denotes the similaritycorrosion betweencurrent pixelsdensity of the coated sample (A/cm²), and j0 is the corrosion current density of the blank sample (i.e., pure epoxy resin) (A/cm²).
In Equation (2), η represents the impedance efficiency, Ri denotes the impedance value of the coated sample (Ω/cm²), and R0 is the impedance value of the blank sample (Ω/cm²).
3. Results and Discussion
3.1 Microstructural Analysis
The morphologies of the EP, HEO-1, HEO-2, and HEO-3 samples were examined using scanning electron microscopy (SEM), as shown in Figure 1. Numerous large bubbles are present inside the EP sample (Figure 1a). This is attributed to the high viscosity of the pure epoxy system, which traps air during stirring, and the entrapped air is unable to escape easily. The bubble control in the originalHEO-1 image;sample (Figure 1b) is thesimilar searchto windowthat in EP, with a considerable number of pixelbubbles observed. ;This is due to the insufficient filler content, which leads to limited dispersion in the resin and an inability to effectively suppress bubble formation during mixing and curing. The HEO-2 sample (Figure 1c) exhibits the fewest and smallest internal bubbles, with the most uniform and complete structure. This improvement is attributed to the filteredoptimal image.
Figurewhich 3moderates Schematicthe illustrationviscosity of the non-localcoating, meansfacilitates bubble escape, and suppresses bubble generation. The HEO-3 sample (NLM)Figure filtering1d) principlealso demonstrates good bubble control but remains inferior to HEO-2. This is because the excessive filler addition increases slurry viscosity and reduces fluidity, hindering bubble removal and leading to partial bubble retention.
Figure 1. SEM images of the composite coating2:(a) EP; (b) HEO-1; (c) HEO-2; (d) HEO-3.
3.2 Polarization Curve Analysis
The methodpolarization curves and corresponding data are presented in Figure 2 and Table 1. As shown in Figure 2 and Table 1, compared with the pure epoxy coating, the coatings containing HEO fillers exhibit a positive shift in corrosion potential and a decrease in corrosion current density, indicating improved anticorrosion performance. Among them, the HEO-2 coating shows a more positive corrosion potential and the lowest corrosion current density, demonstrating the highest anticorrosion efficiency. Even after prolonged exposure to the corrosive medium, the HEO-2 sample maintains excellent anticorrosion performance, suggesting that 2wt% HEO filler achieves good dispersion within the coating and effectively inhibits the penetration of corrosive species.
Figure 2. Polarization curves of samples with different coatings without immersion (a) and immersed for determining10 the similarity between two neighborhood windows is to calculate the mean squared errordays (MSE)b).
Table them:1. Polarization curve fitting data of different coating samples.
| Coating sample | j /( |
E/V | P (%) | |
| EP | 0 | 1.730×10-7 | -1.019 | - |
| 10 | 8.013×10-7 | -1.021 | - | |
| HEO-1 | 0 | 1.308×10-8 | -0.757 | 92.43 |
| 10 | 1.416×10-8 | -0.517 | 91.82 | |
| HEO-2 | 0 | 1.059×10-9 | -0.191 | 99.39 |
| 10 | 7.669×10-9 | -0.416 | 95.57 | |
| HEO-3 | 0 | 1.424×10-9 | -0.294 | 99.17 |
| 10 | 1.422×10-8 | -0.744 | 91.78 |
3.3 Electrochemical Impedance Analysis
Here,The electrochemical impedance data are presented in Figure 3 and Table 2. Figure 3 and Table 2 clearly illustrate the performance differences among the coatings. Among the composite coatings, HEO-2 exhibits the highest impedance efficiency, reaching 98.63% initially and remaining at 91.75% after 10 days of immersion. Compared with the other samples, HEO-2 consistently shows the best impedance values and efficiency before and after immersion, indicating that the incorporation of 2wt% HEO provides superior anticorrosion performance, effectively protecting the substrate from corrosion and extending the coating service life. The HEO-1 coating demonstrates an initial impedance efficiency of 91.26%, which decreases significantly to 40.69% after 10 days of immersion. This suggests that 1wt% HEO is insufficient to notably enhance the corrosion protection capability of the coating. Combined with the SEM observations, it can be inferred that the low filler content leads to inadequate dispersion, resulting in limited reinforcement and modification effects. The HEO-3 coating shows an initial impedance efficiency of 96.71% and retains 90.62% after 10 days of immersion, indicating that 3wt% HEO significantly improves anticorrosion performance. However, compared with HEO-2, excessive filler addition leads to diminished efficiency gains and potential material waste, suggesting that 2wt% is the normalizationoptimal factor,loading whichfor isachieving thebalanced sumperformance and economic efficiency.
Figure 3. Nyquist plot of allsamples weights;with different is
thecoatings meanwithout squaredimmersion error;(a) and isimmersed thefor filtering10 coefficient.days The(b).
Table the2. valueElectrochemical impedance data of different ,
thecoating better the denoising effect, but the image becomes more blurred. Conversely, the smaller the value of , the worse the denoising effect, but the less distortion after denoising.
The basic idea of histogram equalization is to perform a nonlinear mapping of image pixel values to make their grayscale distribution more uniform. However, traditional histogram equalization globally stretches the grayscale histogram of the entire image, which may excessively enhance noise in low-contrast areas and lead to the loss of details in high-brightness regions. When histogram equalization is applied to terahertz images, which are low signal-to-noise ratio (SNR) images, the noise is significantly amplified, resulting in salt-and-pepper noise or artifacts. Contrast-limited adaptive histogram equalization (CLAHE)[7] is an improved version of histogram equalization that prevents the issue of excessive noise enhancement. CLAHE limits the contrast within each local region after dividing the image into blocks, thereby avoiding the introduction of excessive noise caused by overly high contrast.
CLAHE sets a threshold for the original image’s histogram, and if the grayscale of a certain bin exceeds this threshold, it is clipped. The excess values are then evenly distributed across the available grayscale levels, as shown in Figure 4. Additionally, to avoid blocky discontinuities caused by image segmentation, bilinear interpolation is used to reconstruct the pixel grayscale values.
Figure 4 Schematic illustration of CLAHE principle
As shown in Figure 5, the background of the terahertz image processed by NLM and CLAHE is significantly cleaner, with a substantial reduction in noise. The readability of weak signal areas has been notably improved; low-contrast features such as bubbles, inclusions, and cracks are more pronounced. Additionally, edge and texture information is better preserved, avoiding the blurring issues typically associated with traditional filtering methods.
Figure 5 Preprocessing workflow diagram
The SRCNN network in the second part is primarily used to enhance the preprocessed images. Unlike the traditional SRCNN[8], the SRCNN in this study uses a 7×7×64 convolutional kernel and a Rectified Linear Unit (ReLU, Max(0, x)) in the first layer to extract features and obtain low-resolution features. In the second layer, a 5×5×32 convolutional kernel is employed to nonlinearly map the low-resolution features to 32 sets of high-resolution features. In the third layer, a 5×5×1 convolutional kernel is used to integrate the high-resolution features and generate the final high-resolution image.
In this study, low-resolution terahertz images with c channels and height and width dimensions of h and w, respectively, are used as the input to the SRCNN, as shown in Figure 6. The first convolutional layer (Conv1) is used to extract low-resolution features, with a convolutional kernel size of f1×f1, n1 filters, and a ReLU activation function. To ensure that the image size remains unchanged after convolution, padding should be applied during the convolution process, with the padding size set to padding = f1//2. After Conv1, the output feature map has a size of n1×h×w.samples.
| Coating sample | R/( |
η(%) | |
| EP | 0 | 8.653×105 | - |
| 10 | 5.573×105 | - | |
| HEO-1 | 0 | 9.902×106 | 91.26 |
| 10 | 1.459×106 | 40.69 | |
| HEO-2 | 0 | 6.324×107 | 98.63 |
| 10 | 1.049×107 | 91.75 | |
| HEO-3 | 0 | 2.637×107 | 96.71 |
| 10 | 9.226×106 | 90.62 |
3.4 Hydrophobicity Test
The secondwater layerabsorption data obtained by the gravimetric method are presented in Figure 4. As shown in Figure 4, the water absorption rates of the SRCNNepoxy network,composite Conv2,coatings iscontaining usedHEO tofillers establishare thesignificantly mappinglower relationshipthan between low-resolution and high-resolution features. It maps the n1 low-resolution feature vectors from Conv1 to n2 high-dimensional feature vectors, which represent the featuresthat of the high-resolutionpure image.epoxy The convolutional kernel size of Conv2 is f2×f2, with n2 filters,coating, and the activationincrease functionin water absorption over time is ReLU.also Paddingmuch slower. This improvement is applied with a size of padding = f2//2. After passing through Conv2, the output feature map has a size of n2×h×w.
The third layer of the SRCNN network, Conv3, is used to reconstruct the high-resolution image. Conv3 can be understood as a set of linear filters, and the average of the filtered results represents the predicted image, with the output being the final reconstructed image. The convolutional kernel size of Conv3 is f3*f3, with c filters, and padding is applied with a size of padding = f3//2. After passing through Conv3, the output is a high-resolution image with a size of c×h×w.
Unlike the traditional SRCNN, in this study, the convolutional kernel size in the first layer is f1×f1 = 7×7, with padding = 3. In the second layer, the convolutional kernel size is f2×f2 = 5×5, with padding = 2. The convolutional kernel size in the third layer is the same as that in the traditional SRCNN, f3×f3 = 5×5. This design is relatedattributed to the particularitiesincorporation of terahertzHEO images.
Figurepartially 6: SRCNN Network Diagram
3. Material and method
The terahertz time-domain spectroscopy (THz-TDS) imaging system employed in this study, provided by Qingdao Qingyuan Fengda Terahertz Technology Co., Ltd., consists of four primary components: a computer, main unit, imaging module, and a two-dimensional scanning platform. The system operates within a frequency bandwidth of 0.1-4.5 THz, with three selectable pulse scanning speeds (120ps@25Hz, 90ps@30Hz, and 300ps@10Hz). It demonstrates a lateral resolution of 1 mm, thickness detection range of 30 μm-9 mm, thickness measurement accuracy of ±2 μm, and an imaging field of view (FOV) of 100mm×100mm.
Epoxy resin, recognized for its high dielectric strength and corrosion resistance, has found extensive industrial applications as a critical insulating material in power grid systems. This study selected epoxy resin asfill the targetmicro-voids insulating material. Specimens containing artificially induced defects (gas bubbles and embedded inclusions) were prepared through controlled gas injectiongenerated during the curing process of the epoxy matrix, resulting in a denser coating structure that effectively inhibits water penetration and deliberateenhances inclusionhydrophobic performance. Furthermore, the high hardness, excellent corrosion resistance, and outstanding chemical stability of foreignHEO particles.contribute Theto specimensgreater wereresistance fabricatedagainst withintrusion dimensionsby corrosive molecules, thereby maintaining the structural integrity of 50mm×50mm×3mm.the Thecoating experimentaland setupfurther involvedimproving positioningits hydrophobicity.
Figure 4. Water absorption of different coating samples onafter a lifting platform and acquiring terahertz signals through transmission-mode THz-TDS. A two-dimensional scanning platform performed raster scanning with a step size of 0.2mm, yielding 272×272 pixel images.
The acquisition of terahertz images presents notable challenges, including prolonged imaging durations (requiring no less than 40 minutes per specimen in this study). Furthermore, terahertz nondestructive testingsoaking for insulatingdifferent materials remains in its nascent stages with insufficient data accumulation. These constraints make the establishment of large-scale terahertz image training datasets impractical. To address this limitation, we utilized the public DIV2K dataset for network training while reserving 10 acquired terahertz images for testing.
Following model architecture development and dataset preparation, network training was implemented using PyTorch 2.4.0 framework under Python 3.7 environment. Training computations were executed on an Intel Xeon 6133 processor coupled with an NVIDIA RTX 4080S GPU. The super-resolution reconstruction network was configured with 4× magnification factor, initial learning rate of 10-4, and batch size of 16. The model underwent 500 training epochs using Adam optimization algorithm for parameter updates.time.
4.3.5 ResultsAnticorrosion andMechanism analysisAnalysis
The followinganticorrosion imagemechanism demonstratesof the experimentalepoxy resultscomposite ofcoating imageis super-resolutionillustrated reconstruction.in Figure 7(a)5. showsThe corrosion protection primarily arises from the originalphysical terahertzbarrier image,effect Figure 7(b) displays the image processedprovided by the classicalanticorrosive SRCNNfillers. [7]Pure network,epoxy Figureresin 7(c)has presentshigh viscosity, which facilitates air entrapment during mixing with the imagecuring processedagent, byleading to the SRGANformation [9]of network,micropore. andIn Figureaddition, 7(d)solvent showsevaporation theduring imageepoxy processedcuring byalso thecontributes SRCNNto networkmicropore proposed in this paper.formation. As shown in Figure 7(5(a), when corrosive species penetrate the originalcoating, terahertzthey imagecan reach the metal substrate through these micropore, initiating corrosion reactions upon contact. Therefore, pure epoxy resin exhibits noticeablerelatively artifacts,poor corrosion resistance in electrochemical tests. Figure 5(b) presents the schematic diagram of the corrosion protection mechanism after incorporating HEO fillers. As an anticorrosive filler, HEO possesses high hardness, strong corrosion resistance, and excellent chemical stability owing to its lattice distortion effect, sluggish diffusion effect, and high-entropy effect. The appropriate addition of HEO not only suppresses bubble formation and fills the voids in the epoxy matrix, but thesealso artifactsacts areas a physical barrier, creating a “tortuous path” or “maze effect” that significantly improveddelays the permeation of corrosive molecules toward the substrate.
Figure 5. Schematic diagram of corrosion resistance mechanism of composite coatings (a) pure epoxy resin coating (b) epoxy resin composite coating with HEO.
4. Conclusion
Electrochemical measurements demonstrated that the HEO-2 coating exhibits excellent corrosion resistance. Before immersion, the corrosion protection efficiency reached 99.39%. After immersion in Figures3.5wt% 7(b)NaCl andsolution (d).for In10 Figure 7(c),days, the sharpnesscoating andretained contrasta athigh theprotection imageefficiency edgesof are95.57%. visiblyThe enhanced,impedance butefficiency some distortion and noise are introduced after SRGAN processing. Subjectively, the difference between Figures 7(b) and 7(d) is small, butobtained from the zoomed-inNyquist view,plots was 98.63%, and remained at 91.75% after 10 days of immersion.
Hydrophobicity tests further confirmed that the textureHEO-2 epoxy composite coating possesses outstanding water-repellent properties. The initial water absorption rate was 2.37%, and only slightly increased to 2.72% after 10 days of immersion in Figure3.5wt% 7(d)NaCl issolution, clearerindicating thanthat the HEO-2 composite coating has a denser microstructure, resulting in Figureimproved 7(b). In contrast, Figure 7(b) exhibits some mosaic effects, which negatively impact its overall quality.
Figure 7: Terahertz Images of Epoxy Resin Samples
(a) Original Image(b) SRCNN(c) SRGAN(d) Ours
The aforementioned three algorithms have each demonstrated a degree of enhancement on terahertz images. In addition to subjective evaluation[10], a quantitative comparison of their effectiveness is required. To objectively compare the performance of these algorithms, Peak Signal-to-Noise Ratio (PSNR)hydrophobicity and Structuralenhanced Similaritycorrosion Index (SSIM) were selected as evaluation criteria for assessing enhancement quality. PSNR, one of the most widely used metrics in image processing, represents the ratio between the maximum possible signal power and the power of corrupting noise that affects fidelity. A higher PSNR value indicates superior image quality. SSIM, another prevalent image similarity metric, emphasizes structural information in quality assessment, aligning with human visual perception. Thus, SSIM better approximates human judgment of image quality, where values closer to 1 indicate lower distortion.protection.
As showna inhigh-entropy Figureoxide, 8,Y2(Ti0.2Zr0.2Hf0.2Ce0.2V0.2)2O7 exhibits excellent structural stability, high hardness, and superior corrosion resistance. Its incorporation into the proposedepoxy algorithmmatrix achievessignificantly smoother textures and more pronounced edges. In contrast, images processed byenhances the conventional SRCNN algorithm exhibit mosaic artifacts that degrade visual quality. Meanwhile, the SRGAN network, with its more complex architecture, was trained exclusively on open-source optical image datasets, making it more suitable for optical image reconstruction. Comprehensive analysis of Figure 8 and Table 1 leads to the conclusion that the improved SRCNN achieves optimal enhancement performance.
The superioranticorrosion performance of the proposedcomposite algorithmcoating. stemsThe fromcombination twoof architecturalinorganic innovations:fillers First,with organic coatings represents an important research direction for advanced protective coatings, offering broad application prospects and warranting further investigation.
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J Chen, X Li, et al. (2024) Influence of
acorrosion5×5inhibitorsconvolutionalonkernelagingin the subsequent layer expands the receptive field[11], facilitating reconstruction of intricate textures. This dual optimization effectively mitigates checkerboard artifacts and improves edge continuity compared to conventional approaches.Figure 8: Magnified Terahertz Image Details of Epoxy Resin Samples (a) Original Image(b) SRCNN(c) SRGAN(d) OursTable 1: Comparison of Reconstruction Results for Three NetworksProjectPSNR/dBSSIMSRCNN27.620.925SRGAN21.320.754Ours27.390.9285. ConclusionsThis paper proposes a novel super-resolution reconstruction network that integrates traditional image processing algorithms with SRCNN to address the challenges of high noise, low contrast, and limited resolution in terahertz images, thereby enhancing the precision and accuracy of non-destructive testing for insulating materials in engineering applications. Terahertz imagesmechanism of epoxy resinsamples containing bubble and inclusion defects were employed as experimental inputs. The framework first preprocesses the images using NLM and CLAHE algorithms. The preprocessed images are subsequently fed into the modified SRCNN networkcoatings forsuper-resolutioncopperreconstruction.62Experimentalalloyresultsindemonstratesimulatedthatmarinetheenvironment.proposedCorrosionalgorithmReviews.,effectively reduces artifacts, enriches image details, and improves spatial resolution compared to conventional approaches.43(4):457-467.Acknowledgement -
doubleThisGataworkJosephwasA.supported(2023)byMethodologytheforScience and Technology Projectdevelopment ofChinasmartSouthernepoxyPowercoatingsGridincorporatedCo.,withLtd.Ethylenediamine-N, N'-disuccinic ac-id (GrantEDDS)No.layeredGDKJXM20222546).
hydroxidesReferences[1](LDHs)YufanforW.corrosionResearch on the Impactprotection ofTemperatureXC38Gradientcarbononsteel.theMaterials.InsulationINSABreakdowndeCharacteristics of Epoxy Resin and Its Phase Field Simulation [D]. Tianjin University, 2022. (in Chinese).Lyon.[2]
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