Nothing Special   »   [go: up one dir, main page]

You seem to have javascript disabled. Please note that many of the page functionalities won't work as expected without javascript enabled.
 
 
Sign in to use this feature.

Years

Between: -

Subjects

remove_circle_outline
remove_circle_outline
remove_circle_outline
remove_circle_outline
remove_circle_outline
remove_circle_outline

Journals

Article Types

Countries / Regions

Search Results (84)

Search Parameters:
Keywords = energy spectrum entropy

Order results
Result details
Results per page
Select all
Export citation of selected articles as:
27 pages, 543 KiB  
Article
Modification of Premises for the Black Hole Information Paradox Caused by Topological Constraints in the Event Horizon Vicinity
by Janusz Edward Jacak
Entropy 2024, 26(12), 1035; https://doi.org/10.3390/e26121035 - 29 Nov 2024
Viewed by 212
Abstract
We demonstrate that at the rim of the photon sphere of a black hole, the quantum statistics transition takes place in any multi-particle system of indistinguishable particles, which passes through this rim to the inside. The related local departure from Pauli exclusion principle [...] Read more.
We demonstrate that at the rim of the photon sphere of a black hole, the quantum statistics transition takes place in any multi-particle system of indistinguishable particles, which passes through this rim to the inside. The related local departure from Pauli exclusion principle restriction causes a decay of the internal structure of collective fermionic systems, including the collapse of Fermi spheres in compressed matter. The Fermi sphere decay is associated with the emission of electromagnetic radiation, taking away the energy and entropy of the falling matter without unitarity violation. The spectrum and timing of the related e-m radiation agree with some observed short giant gamma-ray bursts and X-ray components of the luminosity of quasars and of short transients powered by black holes. The release of energy and entropy when passing the photon sphere rim of a black hole significantly modifies the premises of the information paradox at the falling of matter into a black hole. Full article
(This article belongs to the Special Issue The Black Hole Information Problem)
21 pages, 6351 KiB  
Article
The Influence of Structure Optimization on Vortex Suppression and Energy Dissipation in the Draft Tube of Francis Turbine
by Xiaoxu Zhang, Cong Nie and Zhumei Luo
Processes 2024, 12(10), 2249; https://doi.org/10.3390/pr12102249 - 15 Oct 2024
Viewed by 742
Abstract
Under partial load operating conditions, vortex rope generation in the draft tube of a Francis turbine is considered one of the main reasons for hydro unit vibration. In this paper, a Francis turbine HLA551-LJ-43 in the laboratory was taken as a prototype. Numerical [...] Read more.
Under partial load operating conditions, vortex rope generation in the draft tube of a Francis turbine is considered one of the main reasons for hydro unit vibration. In this paper, a Francis turbine HLA551-LJ-43 in the laboratory was taken as a prototype. Numerical simulations of the entire flow passage were carried out. Four different hydro-turbines were chosen to analyze the effect of vortex suppression, which were named the prototype turbine (N-J), the turbine with J-grooves installed on its conical section (W-J), the one with extending runner cone (C), and the one that considered the J-grooves and the extending runner cone at the same time (J+C). Under the part load conditions in which the vortex rope is easily generated (0.4–0.8 times design flow QBEP), the spectrum characteristics of pressure fluctuation, the morphology of vortex rope, and the energy dissipation based on the entropy production theory in the draft tube were studied. The results show that the three optimized structures W-J, C, and J+C could reduce the pressure pulsation in the conical section of the draft tube, weaken the eccentricity of the vortex rope, and decrease the energy losses in the runner and draft tube. It is worth mentioning that the turbine with a J+C optimized structure had the most potent effect on vortex suppression and energy dissipation. Primarily when operating in deep partial load (DPL) conditions, the efficiency of the turbine with a J+C optimized structure was increased by 13.7% compared to the prototype turbine, and the main frequency amplitude of the pressure pulsation in the draft tube was reduced to 32% of the prototype. Full article
(This article belongs to the Section Process Control and Monitoring)
Show Figures

Figure 1

Figure 1
<p>Prototype hydro turbine HLA551-LJ-43.</p>
Full article ">Figure 2
<p>Three-dimensional model of the prototype turbine.</p>
Full article ">Figure 3
<p>Grid independence verification.</p>
Full article ">Figure 4
<p>The y plus of the Francis turbine blade.</p>
Full article ">Figure 5
<p>Unstructured hexahedral grids of each flow component.</p>
Full article ">Figure 6
<p>The layout of the modification measures of W-J and C, the location of the monitoring points, and the monitoring surface.</p>
Full article ">Figure 7
<p>Pressure fluctuation at monitoring points TS2 of the prototype and the three structural optimization measures under DPL and PL conditions, listed as: (<b>a</b>) <span class="html-italic">Q</span>* = 53% (DPL); (<b>b</b>) <span class="html-italic">Q</span>* = 69% (PL).</p>
Full article ">Figure 8
<p>Pressure fluctuation spectrogram at monitoring points TS2 of the prototype and the three structural optimization measures under DPL and PL conditions, listed as: (<b>a</b>) Q* = 53% (DPL); (<b>b</b>) Q* = 69% (PL).</p>
Full article ">Figure 9
<p>The distribution of the circumferential and axial velocity of the prototype and the three structural optimization measures under DPL and PL conditions, listed as: (<b>a</b>) <span class="html-italic">Q</span>* = 53% (DPL); (<b>b</b>) <span class="html-italic">Q</span>* = 69% (PL).</p>
Full article ">Figure 10
<p>The vortex rope zone of the prototype and the three structural optimization measures under DPL and PL conditions, listed as: (<b>a</b>) <span class="html-italic">Q</span>* = 53% (DPL); (<b>b</b>) <span class="html-italic">Q</span>* = 69% (PL).</p>
Full article ">Figure 11
<p>The streamlines of section TP1 of the draft tube under DPL and PL conditions, listed as: (<b>a</b>) <span class="html-italic">Q</span>* = 53% (DPL); (<b>b</b>) <span class="html-italic">Q</span>* = 69% (PL).</p>
Full article ">Figure 12
<p>LEPR distribution on the outlet of runner and draft tube of different modification measures under DPL operating conditions (<span class="html-italic">Q</span>* = 53%), listed as: (<b>a</b>) N-J; (<b>b</b>) W-J; (<b>c</b>) C; (<b>d</b>) C+J.</p>
Full article ">Figure 13
<p>Hydraulic losses of four turbine models under different operating conditions.</p>
Full article ">Figure 14
<p>Efficiency of four turbine models under different operating conditions.</p>
Full article ">
15 pages, 6073 KiB  
Article
Underwater Small Target Detection Method Based on the Short-Time Fourier Transform and the Improved Permutation Entropy
by Jing Zhou, Baoan Hao, Yaan Li and Xiangfeng Yang
Acoustics 2024, 6(4), 870-884; https://doi.org/10.3390/acoustics6040048 - 10 Oct 2024
Viewed by 833
Abstract
In the realm of underwater active target detection, the presence of reverberation is an important factor that significantly impacts the efficacy of detection. This article introduces the improved permutation entropy algorithm into the analysis of active underwater acoustic signals. Based on the significant [...] Read more.
In the realm of underwater active target detection, the presence of reverberation is an important factor that significantly impacts the efficacy of detection. This article introduces the improved permutation entropy algorithm into the analysis of active underwater acoustic signals. Based on the significant difference between the improved permutation entropy in the frequency domain and the time domain, a frequency-domain-improved permutation entropy detection algorithm is proposed. The performance of this algorithm and the energy detection algorithm are compared and analyzed under the same conditions. The results show that the spectral entropy detector is about 2.7 dB better than the energy detector, realized via active small target signal detection under a reverberation background. At the same time, based on the characteristics of improved permutation entropy changing with the length of processed data, the short-time Fourier transform is integrated into frequency domain entropy detection to obtain distance and velocity information of the target. To validate the proposed methods, comparative analysis experiments were executed utilizing actual experiment data. The outcomes of both simulation and actual experiment data processing demonstrated that the sliding entropy feature detection method for signal spectrum has a small computational complexity and can quickly determine whether there is a target echo in the receive data. The two-dimensional entropy feature detection method for short-time signal spectra was found to effectively mitigate the impact of reverberation intensity and while enhancing the prominence of the target signal, thereby yielding a more robust detection outcome. Full article
(This article belongs to the Special Issue Vibration and Noise (2nd Edition))
Show Figures

Figure 1

Figure 1
<p>Simulation results of reverberation and target echo signals. (<b>a</b>) Reverberation signal; (<b>b</b>) normalized reverberation signal; (<b>c</b>) normalized reverberation signal after adding target echo signal; (<b>d</b>) time-frequency diagram of the target echo signal and reverberation.</p>
Full article ">Figure 1 Cont.
<p>Simulation results of reverberation and target echo signals. (<b>a</b>) Reverberation signal; (<b>b</b>) normalized reverberation signal; (<b>c</b>) normalized reverberation signal after adding target echo signal; (<b>d</b>) time-frequency diagram of the target echo signal and reverberation.</p>
Full article ">Figure 2
<p>IPE and PE values of noise with different bandwidths in the time domain.</p>
Full article ">Figure 3
<p>IPE and PE values of noise with different bandwidths in the frequency domain.</p>
Full article ">Figure 4
<p>Spectral entropy detection and energy detection performance curve.</p>
Full article ">Figure 5
<p>Variation of spectral entropy detection performance with data time length under different SNR conditions.</p>
Full article ">Figure 6
<p>IPE result of the signal spectrum when the signal-to-noise ratio is 0 dB. (<b>a</b>) IPE value of the spectrum under a sliding window; (<b>b</b>) STFT for IPE value.</p>
Full article ">Figure 7
<p>IPE result of the signal spectrum when the signal-to-noise ratio is −15 dB. (<b>a</b>) IPE value of the spectrum under a sliding window; (<b>b</b>) STFT for IPE value.</p>
Full article ">Figure 8
<p>The time-frequency analysis diagram of reverberation with noise.</p>
Full article ">Figure 9
<p>Entropy characteristics of the power spectrum in different time and frequency frames when only Gaussian white noise is added. (<b>a</b>) Entropy characteristics of the power spectrum in time frames; (<b>b</b>) entropy characteristics of the power spectrum in frequency frames.</p>
Full article ">Figure 10
<p>Entropy characteristics of the power spectrum in different time and frequency frames when the signal-to-noise ratio is 0 dB. (<b>a</b>) Entropy characteristics of the power spectrum in time frames; (<b>b</b>) entropy characteristics of the power spectrum in frequency frames.</p>
Full article ">Figure 11
<p>Active acquisition of time-domain waveforms and time-frequency maps without target signals.</p>
Full article ">Figure 12
<p>Active acquisition of time-domain waveforms and time-frequency maps when there is a target signal.</p>
Full article ">Figure 13
<p>Detection result without target signal. (<b>a</b>) Entropy characteristics of the power spectrum in time frames; (<b>b</b>) entropy characteristics of the power spectrum in frequency frames.</p>
Full article ">Figure 14
<p>Detection results with a target signal. (<b>a</b>) Entropy characteristics of the power spectrum in time frames; (<b>b</b>) entropy characteristics of the power spectrum in frequency frames.</p>
Full article ">Figure 15
<p>Detection results for different distance targets. (<b>a</b>) Entropy characteristics of the power spectrum in time frames; (<b>b</b>) entropy characteristics of the power spectrum in frequency frames.</p>
Full article ">
10 pages, 1356 KiB  
Article
Entropy and Negative Specific Heat of Doped Graphene: Topological Phase Transitions and Nernst’s Theorem Revisited
by L. Palma-Chilla, Juan A. Lazzús and J. C. Flores
Entropy 2024, 26(9), 771; https://doi.org/10.3390/e26090771 - 10 Sep 2024
Cited by 1 | Viewed by 704
Abstract
This study explores the thermodynamic properties of doped graphene using an adapted electronic spectrum. We employed the one-electron tight-binding model to describe the hexagonal lattice structure. The dispersion relation for graphene is expressed in terms of the hopping energies using a compositional parameter [...] Read more.
This study explores the thermodynamic properties of doped graphene using an adapted electronic spectrum. We employed the one-electron tight-binding model to describe the hexagonal lattice structure. The dispersion relation for graphene is expressed in terms of the hopping energies using a compositional parameter that characterizes the different dopant atoms in the lattice. The focus of the investigation is on the impact of the compositions, specifically the presence of dopant atoms, on the energy spectrum, entropy, temperature, and specific heat of graphene. The numerical and analytical results reveal distinct thermodynamic behaviors influenced by the dopant composition, including topological transitions, inflection points in entropy, and specific heat divergences. In addition, the use of Boltzmann entropy and the revision of Nernst’s theorem for doped graphene are introduced as novel aspects. Full article
(This article belongs to the Section Thermodynamics)
Show Figures

Figure 1

Figure 1
<p>(<b>a</b>) Representation of the honeycomb lattice structure of a doped graphene, including the elementary vectors <math display="inline"><semantics> <mrow> <msub> <mrow> <mi>a</mi> </mrow> <mrow> <mn>1</mn> </mrow> </msub> </mrow> </semantics></math> and <math display="inline"><semantics> <mrow> <msub> <mrow> <mi>a</mi> </mrow> <mrow> <mn>2</mn> </mrow> </msub> </mrow> </semantics></math>, and the nearest-neighbor vectors <math display="inline"><semantics> <mrow> <msub> <mrow> <mi>δ</mi> </mrow> <mrow> <mn>1</mn> </mrow> </msub> </mrow> </semantics></math>, <math display="inline"><semantics> <mrow> <msub> <mrow> <mi>δ</mi> </mrow> <mrow> <mn>2</mn> </mrow> </msub> </mrow> </semantics></math>, and <math display="inline"><semantics> <mrow> <msub> <mrow> <mi>δ</mi> </mrow> <mrow> <mn>3</mn> </mrow> </msub> </mrow> </semantics></math>. White and black atoms represent the C and dopant atoms in the graphene lattice, respectively. (<b>b</b>) Graphical representation of the spectrum of doped graphene <math display="inline"><semantics> <mrow> <mi>γ</mi> <mo> </mo> <mo>~</mo> <mo> </mo> <mn>0.92</mn> </mrow> </semantics></math> as a contour map of the energy dispersion obtained from Equation (3). As observed, the spectrum exhibits a double topological transition with energy levels that cross the entire cell (and the lattice) and are located between both topological transitions (note the black levels). In contrast, pristine graphene <math display="inline"><semantics> <mrow> <mi>γ</mi> <mo>=</mo> <mn>1</mn> </mrow> </semantics></math> exhibits only one topological transition when the energy levels pass from the six Dirac cones (lower energy levels) to only one central figure similar to a dome with upper energy levels (see the inner panel).</p>
Full article ">Figure 2
<p>(<b>a</b>) Associated Boltzmann entropy <math display="inline"><semantics> <mrow> <msub> <mrow> <mi>S</mi> </mrow> <mrow> <mi>B</mi> </mrow> </msub> <mo>(</mo> <mi>E</mi> <mo>)</mo> </mrow> </semantics></math> for the doped graphene spectrum as a function of dimensionless energy <math display="inline"><semantics> <mrow> <mi>E</mi> </mrow> </semantics></math>. At a well-defined point, for any compositional parameter <math display="inline"><semantics> <mrow> <mi>γ</mi> </mrow> </semantics></math>, the entropy exhibits a gap, and around this gap, there are two inflection points on the curve. For a better visualization, the inner panel shows a zoom of the gaps of the entropy curve. (<b>b</b>) Temperature <math display="inline"><semantics> <mrow> <mi>T</mi> <mfenced separators="|"> <mrow> <mi>E</mi> </mrow> </mfenced> </mrow> </semantics></math> for the mentioned three cases as a function of dimensionless energy. Observe the existence of negative temperatures for “high-energy” ranges, and discontinuity in correspondence with the non-differentiable points of the entropy curve.</p>
Full article ">Figure 2 Cont.
<p>(<b>a</b>) Associated Boltzmann entropy <math display="inline"><semantics> <mrow> <msub> <mrow> <mi>S</mi> </mrow> <mrow> <mi>B</mi> </mrow> </msub> <mo>(</mo> <mi>E</mi> <mo>)</mo> </mrow> </semantics></math> for the doped graphene spectrum as a function of dimensionless energy <math display="inline"><semantics> <mrow> <mi>E</mi> </mrow> </semantics></math>. At a well-defined point, for any compositional parameter <math display="inline"><semantics> <mrow> <mi>γ</mi> </mrow> </semantics></math>, the entropy exhibits a gap, and around this gap, there are two inflection points on the curve. For a better visualization, the inner panel shows a zoom of the gaps of the entropy curve. (<b>b</b>) Temperature <math display="inline"><semantics> <mrow> <mi>T</mi> <mfenced separators="|"> <mrow> <mi>E</mi> </mrow> </mfenced> </mrow> </semantics></math> for the mentioned three cases as a function of dimensionless energy. Observe the existence of negative temperatures for “high-energy” ranges, and discontinuity in correspondence with the non-differentiable points of the entropy curve.</p>
Full article ">Figure 3
<p>(<b>a</b>) Specific heat <math display="inline"><semantics> <mrow> <mi>C</mi> </mrow> </semantics></math> for doped graphene (with <math display="inline"><semantics> <mrow> <mi>γ</mi> <mo> </mo> <mo>~</mo> <mo> </mo> <mn>0.92</mn> </mrow> </semantics></math> and <math display="inline"><semantics> <mrow> <mi>γ</mi> <mo> </mo> <mo>~</mo> <mo> </mo> <mn>0.86</mn> </mrow> </semantics></math>) as a function of dimensionless energy <math display="inline"><semantics> <mrow> <mi>E</mi> </mrow> </semantics></math> (the pristine case is also included). The inner panel shows a zoom picture around <math display="inline"><semantics> <mrow> <mi>E</mi> <mo>~</mo> <mn>1</mn> </mrow> </semantics></math> exhibiting three points with zero specific heat at <math display="inline"><semantics> <mrow> <mi>T</mi> <mo>~</mo> <mn>0</mn> </mrow> </semantics></math>, one for each compositional parameter <math display="inline"><semantics> <mrow> <mi>γ</mi> </mrow> </semantics></math>. (<b>b</b>) Specific heat as a function of temperature for doped graphene with <math display="inline"><semantics> <mrow> <mi>γ</mi> <mo> </mo> <mo>~</mo> <mo> </mo> <mn>0.92</mn> </mrow> </semantics></math> compared to pristine graphene (details in the text).</p>
Full article ">
13 pages, 2115 KiB  
Article
Uncovering a Genetic Diagnosis in a Pediatric Patient by Whole Exome Sequencing: A Modeling Investigation in Wiedemann–Steiner Syndrome
by Ighli di Bari, Caterina Ceccarini, Maria Curcetti, Carla Cesarano, Anna-Irma Croce, Iolanda Adipietro, Maria Grazia Gallicchio, Grazia Pia Palladino, Maria Pia Patrizio, Benedetta Frisoli, Rosa Santacroce, Maria D’Apolito, Giovanna D’Andrea, Ombretta Michela Castriota, Ciro Leonardo Pierri and Maurizio Margaglione
Genes 2024, 15(9), 1155; https://doi.org/10.3390/genes15091155 - 1 Sep 2024
Viewed by 959
Abstract
Background: Wiedemann–Steiner syndrome (WSS), a rare autosomal-dominant disorder caused by haploinsufficiency of the KMT2A gene product, is part of a group of disorders called chromatinopathies. Chromatinopathies are neurodevelopmental disorders caused by mutations affecting the proteins responsible for chromatin remodeling and transcriptional regulation. The [...] Read more.
Background: Wiedemann–Steiner syndrome (WSS), a rare autosomal-dominant disorder caused by haploinsufficiency of the KMT2A gene product, is part of a group of disorders called chromatinopathies. Chromatinopathies are neurodevelopmental disorders caused by mutations affecting the proteins responsible for chromatin remodeling and transcriptional regulation. The resulting gene expression dysregulation mediates the onset of a series of clinical features such as developmental delay, intellectual disability, facial dysmorphism, and behavioral disorders. Aim of the Study: The aim of this study was to investigate a 10-year-old girl who presented with clinical features suggestive of WSS. Methods: Clinical and genetic investigations were performed. Whole exome sequencing (WES) was used for genetic testing, performed using Illumina technology. The bidirectional capillary Sanger resequencing technique was used in accordance with standard methodology to validate a mutation discovered by WES in all family members who were available. Utilizing computational protein modeling for structural and functional studies as well as in silico pathogenicity prediction models, the effect of the mutation was examined. Results: WES identified a de novo heterozygous missense variant in the KMT2A gene KMT2A(NM_001197104.2): c.3451C>G, p.(Arg1151Gly), absent in the gnomAD database. The variant was classified as Likely Pathogenetic (LP) according to the ACMG criteria and was predicted to affect the CXXC-type zinc finger domain functionality of the protein. Modeling of the resulting protein structure suggested that this variant changes the protein flexibility due to a variation in the Gibbs free energy and in the vibrational entropy energy difference between the wild-type and mutated domain, resulting in an alteration of the DNA binding affinity. Conclusions: A novel and de novo mutation discovered by the NGS approach, enhancing the mutation spectrum in the KMT2A gene, was characterized and associated with WSS. This novel KMT2A gene variant is suggested to modify the CXXC-type zinc finger domain functionality by affecting protein flexibility and DNA binding. Full article
(This article belongs to the Section Human Genomics and Genetic Diseases)
Show Figures

Figure 1

Figure 1
<p>Patient’s characteristics. Features include mild facial dysmorphisms (hypertelorism, epicanthus, wide nasal bridge, and low-set ears), stubby and puffy hands, and hypertrichosis.</p>
Full article ">Figure 2
<p>(<b>A</b>) Electropherograms showing the c.3451C&gt;G variant in the index case. The arrow shows the nucleotide substitution. (<b>B</b>) Schematic representation of the Histone lysine N-methyltransferase 2A (UniProt Q03164) showing the localization of the variant p.R1151G (highlighted with the arrow) found in the proband. The various domains are shown in sequential order from NH2 to COOH: CXXC-type zinc finger (CxxC), plant homeodomain (PHD), Bromodomain, extended plant homeodomain (ePHD), FY-rich N-terminal (FYRN), FY-rich C-terminal (FYRC), Su(Var)3-9 enhancer-of-zestetrithorax (SET) and post-SET. (<b>C</b>) Pedigree of proband with mutation in <span class="html-italic">KMT2A</span> and her family. Circles show females, squares show males. An arrowhead indicates the proband. (<b>D</b>) Alignment of the CXXC-type zinc finger domain (the amino acid location p.1151 is showed in red and indicated by a blue arrow) along different species boxed in light blue.</p>
Full article ">Figure 3
<p>The figure displays the schematic conformation of the original (arginine, R, on the <b>left</b>) and the variant (glycine, G, on the <b>right</b>) amino acid. The backbone, which is the same for each amino acid, is colored in red. The side chain, unique for each amino acid, is colored in black.</p>
Full article ">Figure 4
<p>Amino acids are color-coded based on the change in vibrational entropy after mutation, with blue indicating increased rigidity and red indicating enhanced flexibility of the structure.</p>
Full article ">Figure 5
<p>Comparison of the predicted structures of both (<b>left</b>) wild-type (R1151) and (<b>right</b>) variant (G1151) proteins using the Swiss-Pdb Viewer (<a href="https://spdbv.unil.ch/" target="_blank">https://spdbv.unil.ch/</a> accessed on 15 May 2024). Hydrogen bonds are displayed in light blue dashed lines in the wild-type and mutant proteins. In the structure, the helices are highlighted in red and the strands in yellow. The R1151 (<b>left panel</b>) and G1151 (<b>right panel</b>) products are indicated as green sticks. White sticks indicate DNA.</p>
Full article ">Figure 6
<p>Molecular characterization and 3D modeling of the <span class="html-italic">KMT2A</span> mutational profile. KMT2A is indicated by the white illustration, and R1151 or G1151 are depicted as white sticks. CpG DNA is indicated as orange and light pink lines. Zn ions are indicated by grey spheres. In the insert at the bottom of the figure, a slight perturbation of the local secondary structure of the CXXC domain is highlighted by comparing the variant (blue arrow) and wild-type (orange arrow) proteins.</p>
Full article ">
17 pages, 3646 KiB  
Article
Motion Clutter Suppression for Non-Cooperative Target Identification Based on Frequency Correlation Dual-SVD Reconstruction
by Weikun He, Yichuan Luo and Xiaoxiao Shang
Sensors 2024, 24(16), 5298; https://doi.org/10.3390/s24165298 - 15 Aug 2024
Viewed by 648
Abstract
Non-cooperative targets, such as birds and unmanned aerial vehicles (UAVs), are typical low-altitude, slow, and small (LSS) targets with low observability. Radar observations in such scenarios are often complicated by strong motion clutter originating from sources like airplanes and cars. Hence, distinguishing between [...] Read more.
Non-cooperative targets, such as birds and unmanned aerial vehicles (UAVs), are typical low-altitude, slow, and small (LSS) targets with low observability. Radar observations in such scenarios are often complicated by strong motion clutter originating from sources like airplanes and cars. Hence, distinguishing between birds and UAVs in environments with strong motion clutter is crucial for improving target monitoring performance and ensuring flight safety. To address the impact of strong motion clutter on discriminating between UAVs and birds, we propose a frequency correlation dual-SVD (singular value decomposition) reconstruction method. This method exploits the strong power and spectral correlation characteristics of motion clutter, contrasted with the weak scattering characteristics of bird and UAV targets, to effectively suppress clutter. Unlike traditional clutter suppression methods based on SVD, our method avoids residual clutter or target loss while preserving the micro-motion characteristics of the targets. Based on the distinct micro-motion characteristics of birds and UAVs, we extract two key features: the sum of normalized large eigenvalues of the target’s micro-motion component and the energy entropy of the time–frequency spectrum of the radar echoes. Subsequently, the kernel fuzzy c-means algorithm is applied to classify bird and UAV targets. The effectiveness of our proposed method is validated through results using both simulation and experimental data. Full article
(This article belongs to the Special Issue Radar Target Detection, Imaging and Recognition)
Show Figures

Figure 1

Figure 1
<p>Range-Doppler spectrum with strong motion clutter interference.</p>
Full article ">Figure 2
<p>The block diagram of the method based on frequency correlation dual SVD reconstruction.</p>
Full article ">Figure 3
<p>Block diagram of the bird and UAV targets discrimination against the background of strong motion clutter.</p>
Full article ">Figure 4
<p>Clutter suppression results of a UAV target. (<b>a</b>) The spectrum of the received signal without clutter. (<b>b</b>) The spectrum of the received signal with clutter. (<b>c</b>) The spectrum after clutter suppression (FODS-SVD method). (<b>d</b>) The spectrum after clutter suppression (FEMP-SVD method). (<b>e</b>) Spectrum after clutter suppression (the proposed method).</p>
Full article ">Figure 5
<p>Clutter suppression results of a bird target. (<b>a</b>) The spectrum of the received signal without clutter. (<b>b</b>) The spectrum of the received signal with clutter. (<b>c</b>) The spectrum after clutter suppression (FODS-SVD method). (<b>d</b>) The spectrum after clutter suppression (FEMP-SVD method). (<b>e</b>) Spectrum after clutter suppression (the proposed method).</p>
Full article ">Figure 5 Cont.
<p>Clutter suppression results of a bird target. (<b>a</b>) The spectrum of the received signal without clutter. (<b>b</b>) The spectrum of the received signal with clutter. (<b>c</b>) The spectrum after clutter suppression (FODS-SVD method). (<b>d</b>) The spectrum after clutter suppression (FEMP-SVD method). (<b>e</b>) Spectrum after clutter suppression (the proposed method).</p>
Full article ">Figure 6
<p>Relative power variation comparison after the clutter suppression.</p>
Full article ">Figure 7
<p>Performance comparison of the three methods.</p>
Full article ">Figure 8
<p>(<b>a</b>) The actual radar environment. (<b>b</b>) Radar beam pattern.</p>
Full article ">Figure 9
<p>Clutter suppression results of the bird target. (<b>a</b>) The spectrum of the received signal. (<b>b</b>) Spectrum after clutter suppression (FODS-SVD method). (<b>c</b>) Spectrum after clutter suppression (FEMP-SVD method). (<b>d</b>) Spectrum after clutter suppression (the proposed method).</p>
Full article ">Figure 10
<p>Clutter suppression results of the UAV target. (<b>a</b>) The spectrum of the received signal. (<b>b</b>) Spectrum after clutter suppression (FODS-SVD method). (<b>c</b>) Spectrum after clutter suppression (FEMP-SVD method). (<b>d</b>) Spectrum after clutter suppression (the proposed method).</p>
Full article ">Figure 10 Cont.
<p>Clutter suppression results of the UAV target. (<b>a</b>) The spectrum of the received signal. (<b>b</b>) Spectrum after clutter suppression (FODS-SVD method). (<b>c</b>) Spectrum after clutter suppression (FEMP-SVD method). (<b>d</b>) Spectrum after clutter suppression (the proposed method).</p>
Full article ">Figure 11
<p>Identification results of birds and UAVs. (<b>a</b>) Characteristic spectral energy entropy. (<b>b</b>) Sum of normalized large eigenvalues. (<b>c</b>) Results obtained by kernel fuzzy c-means clustering.</p>
Full article ">
17 pages, 997 KiB  
Article
Spatial Information Entropy-Assisted Integrated Sensing and Communication for Integrated Satellite-Terrestrial Networks
by Xue Wang, Xiaojing Lin and Min Jia
Electronics 2024, 13(15), 3082; https://doi.org/10.3390/electronics13153082 - 4 Aug 2024
Viewed by 669
Abstract
To better meet communication needs, 6G proposes Integrated Satellite-Terrestrial Networks. Integrated Sensing and Communication (ISAC) is one of the key technologies of Integrated Satellite-Terrestrial Networks, which can reduce the energy consumption of the system, improve communication efficiency, and increase the utilization rate of [...] Read more.
To better meet communication needs, 6G proposes Integrated Satellite-Terrestrial Networks. Integrated Sensing and Communication (ISAC) is one of the key technologies of Integrated Satellite-Terrestrial Networks, which can reduce the energy consumption of the system, improve communication efficiency, and increase the utilization rate of spectrum resources. In the existing technology, the Modulated Wideband Converter (MWC) system can provide support for the miniaturization and intelligence of wireless device sensing and communication systems. Therefore, the MWC system can be used as a preliminary application of ISAC technology. However, the reconstruction effect of the conventional MWC system under the influence of noise is not stable. Therefore, we propose a signal processing optimization scheme for the MWC system based on spatial information entropy. First, the subsequent reconstruction algorithm is considered to require the dynamic and flexible processing of the sampled signals to reduce the influence of noise. Second, for the shortcomings of the original Orthogonal Matching Pursuit (OMP) algorithm, the concept of the genetic algorithm is used to optimize the algorithm by constructing the feature factor through spatial information gain and spatial information features. According to the simulation results, compared with the traditional MWC system, the scheme proposed in this paper is improved in all indicators. Full article
Show Figures

Figure 1

Figure 1
<p>MWC System Framework.</p>
Full article ">Figure 2
<p>MWC Sampling Component Framework.</p>
Full article ">Figure 3
<p>CTF Module Framework.</p>
Full article ">Figure 4
<p>Root-mean-square errors of recovered signals at different SNRs.</p>
Full article ">Figure 5
<p>Correlation coefficients of recovered signals at different SNRs.</p>
Full article ">Figure 6
<p>Support set false alarm rates for recovered signals at different SNRs.</p>
Full article ">Figure 7
<p>BERs for recovered signals at different SNRs.</p>
Full article ">Figure 8
<p>Root-mean-square-errors of recovered signals at different SNRs.</p>
Full article ">Figure 9
<p>Correlation coefficients of recovered signals at different SNRs.</p>
Full article ">Figure 10
<p>Support set false alarm rates of recovered signals at different SNRs.</p>
Full article ">Figure 11
<p>When <math display="inline"><semantics> <mrow> <mi>S</mi> <mi>N</mi> <mi>R</mi> <mo>=</mo> <mo>−</mo> <mn>5</mn> </mrow> </semantics></math> and the number of sampling channels is 50, the spectrum of the reconstructed signal is as shown in this figure.</p>
Full article ">Figure 12
<p>BERs of recovered signals at different SNRs.</p>
Full article ">
19 pages, 3640 KiB  
Article
Research on the Skidding Resistance and Attenuation Characteristics of Asphalt Pavement Based on Image Recognition-Analysis Strategy
by Ke Zhang, Dianliang Xi, Yu Zhao, Wei Xie, Wei Zhang and Jiantao Gao
Coatings 2024, 14(6), 749; https://doi.org/10.3390/coatings14060749 - 13 Jun 2024
Viewed by 740
Abstract
To accurately evaluate the skidding resistance of asphalt pavements, a texture imaging device was developed to realize the standardized acquisition of pavement images. Based on the gray-level co-occurrence matrix and multifractal theory of texture structure, the influence of segregation degree and gradation type [...] Read more.
To accurately evaluate the skidding resistance of asphalt pavements, a texture imaging device was developed to realize the standardized acquisition of pavement images. Based on the gray-level co-occurrence matrix and multifractal theory of texture structure, the influence of segregation degree and gradation type on the texture properties of asphalt pavement was studied. Meanwhile, a comprehensive evaluation index of skidding resistance was proposed for asphalt pavement. Furthermore, the attenuation characteristics of the anti-skidding performance for asphalt mixture were explored, and the corresponding attenuation model of asphalt pavement was established. The results show that the segregation degree and gradation type significantly affected the texture parameters and anti-skidding performance of asphalt mixture. Specially, with an increase in the segregation degree of coarse aggregate, the parameters of energy, entropy, and multifractal spectrum width gradually increased, whereas the inertial moment gradually decreased. The variation range of the multifractal spectrum difference initially increased and subsequently decreased. For the texture parameters such as energy, entropy, inertial moment, and multifractal spectrum width Δα, the values of the asphalt mixture with larger nominal maximum particle were higher than those of the mixture with smaller nominal maximum particle, whereas the multifractal spectrum difference value showed the opposite law. In addition, the texture parameters of energy, entropy, and multifractal spectrum width exhibited good linear correlation with the texture depth (TD) of asphalt mixtures with various segregation levels and gradation types. The index based on the texture parameters of energy, entropy, and multifractal spectrum width effectively evaluated the skidding resistance of asphalt pavements, which showed the same trend as the TD with the increase of the abrasion number. The achievement provides an effective solution for the evaluation of skidding resistance and attenuation characteristics of asphalt mixtures. Full article
(This article belongs to the Section Environmental Aspects in Colloid and Interface Science)
Show Figures

Figure 1

Figure 1
<p>Asphalt mixture for the evaluation of texture characteristics.</p>
Full article ">Figure 2
<p>Asphalt mixture for the evaluation of anti-skidding attenuation performance.</p>
Full article ">Figure 3
<p>Sand patch method.</p>
Full article ">Figure 4
<p>Self-developed image acquisition device of the texture structure.</p>
Full article ">Figure 5
<p>Three-dimensional reconstruction model of pavement texture.</p>
Full article ">Figure 6
<p>Anti-skidding attenuation test of asphalt mixture.</p>
Full article ">Figure 7
<p>Texture parameters of asphalt mixture with different segregation degrees.</p>
Full article ">Figure 8
<p>Texture parameters of asphalt mixture with different gradation types.</p>
Full article ">Figure 9
<p>Relationship between the texture parameters and texture depth.</p>
Full article ">Figure 10
<p>Relationship between the comprehensive evaluation index H and texture depth.</p>
Full article ">Figure 11
<p>Comprehensive evaluation index after different abrasion numbers.</p>
Full article ">Figure 12
<p>Texture depth after different abrasion numbers.</p>
Full article ">
15 pages, 11880 KiB  
Article
Medium- and High-Entropy Rare Earth Hexaborides with Enhanced Solar Energy Absorption and Infrared Emissivity
by Hongye Wang, Yanyu Pan, Jincheng Zhang, Kaixian Wang, Liyan Xue, Minzhong Huang, Yazhu Li, Fan Yang and Heng Chen
Materials 2024, 17(8), 1789; https://doi.org/10.3390/ma17081789 - 12 Apr 2024
Cited by 2 | Viewed by 1087
Abstract
The development of a new generation of solid particle solar receivers (SPSRs) with high solar absorptivity (0.28–2.5 μm) and high infrared emissivity (1–22 μm) is crucial and has attracted much attention for the attainment of the goals of “peak carbon” and “carbon neutrality”. [...] Read more.
The development of a new generation of solid particle solar receivers (SPSRs) with high solar absorptivity (0.28–2.5 μm) and high infrared emissivity (1–22 μm) is crucial and has attracted much attention for the attainment of the goals of “peak carbon” and “carbon neutrality”. To achieve the modulation of infrared emission and solar absorptivity, two types of medium- and high-entropy rare-earth hexaboride (ME/HEREB6) ceramics, (La0.25Sm0.25Ce0.25Eu0.25)B6 (MEREB6) and (La0.2Sm0.2Ce0.2Eu0.2Ba0.2)B6 (HEREB6), with severe lattice distortions were synthesized using a high-temperature solid-phase method. Compared to single-phase lanthanum hexaboride (LaB6), HEREB6 ceramics show an increase in solar absorptivity from 54.06% to 87.75% in the range of 0.28–2.5 μm and an increase in infrared emissivity from 76.19% to 89.96% in the 1–22 μm wavelength range. On the one hand, decreasing the free electron concentration and the plasma frequency reduces the reflection and ultimately increases the solar absorptivity. On the other hand, the lattice distortion induces changes in the B–B bond length, leading to significant changes in the Raman scattering spectrum, which affects the damping constant and ultimately increases the infrared emissivity. In conclusion, the multicomponent design can effectively improve the solar energy absorption and heat transfer capacity of ME/HEREB6, thus providing a new avenue for the development of solid particles. Full article
(This article belongs to the Special Issue Design, Processing and Properties of High Entropy Ceramics)
Show Figures

Figure 1

Figure 1
<p>Crystal structure of REB<sub>6</sub>.</p>
Full article ">Figure 2
<p>(<b>a</b>) XRD pattern of ME/HEREB<sub>6</sub> and (<b>b</b>) partial enlargement of the (110) plane.</p>
Full article ">Figure 3
<p>(<b>a</b>–<b>c</b>) Rietveld refinement of the XRD patterns.</p>
Full article ">Figure 4
<p>Samples of (<b>a</b>–<b>c</b>) MEREB<sub>6</sub> and (<b>d</b>–<b>f</b>) HEREB<sub>6</sub>, with their electron diffraction patterns and corresponding inverse fast Fourier transform (IFFT) patterns.</p>
Full article ">Figure 5
<p>Compositional maps from EDS of (<b>a</b>) MEREB<sub>6</sub> and (<b>b</b>) HEREB<sub>6</sub>.</p>
Full article ">Figure 6
<p>Lattice strains calculated based on Williamson–Hall analysis.</p>
Full article ">Figure 7
<p>(<b>a</b>) Raman spectra of LaB<sub>6</sub> and (<b>b</b>) Raman spectra of LaB<sub>6</sub>, MEREB<sub>6</sub>, and HEREB<sub>6</sub>.</p>
Full article ">Figure 8
<p>(<b>a</b>) Reflectance and solar irradiance spectra and (<b>b</b>) solar absorption rates of the LaB<sub>6</sub>, MEREB<sub>6</sub>, and HEREB<sub>6</sub>.</p>
Full article ">Figure 9
<p>(<b>a</b>) Spectrum of the sample emissivity in the range of 0.76–2.5 μm and (<b>b</b>) the normal infrared emissivity in the range of 1–22 μm.</p>
Full article ">
17 pages, 4576 KiB  
Article
Rotating Machinery Fault Diagnosis under Time–Varying Speed Conditions Based on Adaptive Identification of Order Structure
by Xinnan Yu, Xiaowang Chen, Minggang Du, Yang Yang and Zhipeng Feng
Processes 2024, 12(4), 752; https://doi.org/10.3390/pr12040752 - 8 Apr 2024
Cited by 1 | Viewed by 1407
Abstract
Rotating machinery fault diagnosis is of key significance for ensuring safe and efficient operation of various industrial equipment. However, under nonstationary operating conditions, the fault–induced characteristic frequencies are often time–varying. Conventional Fourier spectrum analysis is not suitable for revealing time–varying details, and nonstationary [...] Read more.
Rotating machinery fault diagnosis is of key significance for ensuring safe and efficient operation of various industrial equipment. However, under nonstationary operating conditions, the fault–induced characteristic frequencies are often time–varying. Conventional Fourier spectrum analysis is not suitable for revealing time–varying details, and nonstationary fault feature extraction methods are still in desperate need. Order spectrum can reveal the rotational–speed–related time–varying frequency components as spectral peaks in order domain, thus facilitating fault feature extraction under time–varying speed conditions. However, the speed–unrelated frequency components are still nonstationary after angular–domain resampling, thus causing wide–band features and interferences in the order spectrum. To overcome such a drawback, this work proposes a rotating machinery fault diagnosis method based on adaptive separation of time–varying components and order feature extraction. Firstly, the rotational speed is estimated by the multi–order probabilistic approach (MOPA), thus eliminating the inconvenience of installing measurement equipment. Secondly, adaptive separation of the time–varying frequency component is achieved through time–varying filtering and surrogate test. It effectively eliminates interference from irrelevant components and noise. Finally, a high–resolution order spectrum is constructed based on the average amplitude envelope of each mono–component. It does not involve Fourier transform or angular–domain resampling, thus avoiding spectral leakage and resampling errors. By identifying the fault–related spectral peaks in the constructed order spectrum, accurate fault diagnosis can be achieved. The Rényi entropy values of the proposed order spectrum are significantly lower than those of the traditional order spectrum. This result verifies the effective energy concentration and high resolution of the proposed order spectrum. The results of both numerical simulation and lab experiments confirm the effectiveness of the proposed method in accurately presenting the time–varying frequency components for rotating machinery diagnosing faults. Full article
Show Figures

Figure 1

Figure 1
<p>Schematic diagram of instantaneous rotational speed estimation.</p>
Full article ">Figure 2
<p>Schematic diagram of time–varying filtering.</p>
Full article ">Figure 3
<p>Flowchart of the proposed adaptive high–resolution order spectrum.</p>
Full article ">Figure 4
<p>Traditional order analysis results of multi–harmonic component simulation signal.</p>
Full article ">Figure 5
<p>Accurate estimation of instantaneous speed.</p>
Full article ">Figure 6
<p>Extraction of time–varying component.</p>
Full article ">Figure 7
<p>Accurate identification of frequency order structure.</p>
Full article ">Figure 8
<p>Rolling element bearing test rig configuration.</p>
Full article ">Figure 9
<p>Outer race fault signal of rolling element bearing.</p>
Full article ">Figure 10
<p>Fault diagnosis of rolling element bearing signal.</p>
Full article ">Figure 11
<p>Comparison of Rényi entropy.</p>
Full article ">
15 pages, 2946 KiB  
Article
The EEG-Based Fusion Entropy-Featured Identification of Isometric Contraction Forces under the Same Action
by Bo Yao, Chengzhen Wu, Xing Zhang, Junjie Yao, Jianchao Xue, Yu Zhao, Ting Li and Jiangbo Pu
Sensors 2024, 24(7), 2323; https://doi.org/10.3390/s24072323 - 5 Apr 2024
Cited by 1 | Viewed by 1319
Abstract
This study explores the important role of assessing force levels in accurately controlling upper limb movements in human–computer interfaces. It uses a new method that combines entropy to improve the recognition of force levels. This research aims to differentiate between different levels of [...] Read more.
This study explores the important role of assessing force levels in accurately controlling upper limb movements in human–computer interfaces. It uses a new method that combines entropy to improve the recognition of force levels. This research aims to differentiate between different levels of isometric contraction forces using electroencephalogram (EEG) signal analysis. It integrates eight different entropy measures: power spectrum entropy (PSE), singular spectrum entropy (SSE), logarithmic energy entropy (LEE), approximation entropy (AE), sample entropy (SE), fuzzy entropy (FE), alignment entropy (PE), and envelope entropy (EE). The findings emphasize two important advances: first, including a wide range of entropy features significantly improves classification efficiency; second, the fusion entropy method shows exceptional accuracy in classifying isometric contraction forces. It achieves an accuracy rate of 91.73% in distinguishing between 15% and 60% maximum voluntary contraction (MVC) forces, along with 69.59% accuracy in identifying variations across 15%, 30%, 45%, and 60% MVC. These results illuminate the efficacy of employing fusion entropy in EEG signal analysis for isometric contraction detection, heralding new opportunities for advancing motor control and facilitating fine motor movements through sophisticated human–computer interface technologies. Full article
Show Figures

Figure 1

Figure 1
<p>EEG experimental processes and data processing.</p>
Full article ">Figure 2
<p>Spearman coefficient between different entropies.</p>
Full article ">Figure 3
<p>Accuracy of classification using different entropies as features for 15% and 60% MVCs.</p>
Full article ">Figure 4
<p>Accuracy of entropy feature classification for different subjects at 15% and 60%.</p>
Full article ">Figure 5
<p>Two classification confusion matrixes: sensitivity and specificity.</p>
Full article ">Figure 6
<p>Accuracy of classifying 4-level isometric contractions using different entropies as features. The dotted line indicates the 70% level of classification accuracy.</p>
Full article ">Figure 7
<p>Four-level isometric force classification results.</p>
Full article ">Figure 8
<p>Four confusion matrix classifications and the sensitivity and specificity of each contractile force.</p>
Full article ">
19 pages, 16321 KiB  
Article
A Novel Joint Denoising Method for Hydrophone Signal Based on Improved SGMD and WT
by Tianyu Xing, Xiaohao Wang, Kai Ni and Qian Zhou
Sensors 2024, 24(4), 1340; https://doi.org/10.3390/s24041340 - 19 Feb 2024
Cited by 3 | Viewed by 1242
Abstract
Underwater acoustic technology as an important means of exploring the oceans is receiving more attention. Denoising for underwater acoustic information in complex marine environments has become a hot research topic. In order to realize the hydrophone signal denoising, this paper proposes a joint [...] Read more.
Underwater acoustic technology as an important means of exploring the oceans is receiving more attention. Denoising for underwater acoustic information in complex marine environments has become a hot research topic. In order to realize the hydrophone signal denoising, this paper proposes a joint denoising method based on improved symplectic geometry modal decomposition (ISGMD) and wavelet threshold (WT). Firstly, the energy contribution (EC) is introduced into the SGMD as an iterative termination condition, which efficiently improves the denoising capability of SGMD and generates a reasonable number of symplectic geometry components (SGCs). Then spectral clustering (SC) is used to accurately aggregate SGCs into information clusters mixed-clusters, and noise clusters. Spectrum entropy (SE) is used to distinguish clusters quickly. Finally, the mixed clusters achieve the signal denoising by wavelet threshold. The useful information is reconstructed to achieve the original signal denoising. In the simulation experiment, the denoising effect of different denoising algorithms in the time domain and frequency domain is compared, and SNR and RMSE are used as evaluation indexes. The results show that the proposed algorithm has better performance. In the experiment of hydrophone, the denoising ability of the proposed algorithm is also verified. Full article
Show Figures

Figure 1

Figure 1
<p>The framework of the algorithm combining many methods.</p>
Full article ">Figure 2
<p>Flowchart of the SGMD and improved ISGMD.</p>
Full article ">Figure 3
<p>Target and mixed signals, spectrogram of the target signal. (<b>a</b>) Target and mixed signals. (<b>b</b>) Spectrogram of the target signal.</p>
Full article ">Figure 4
<p>Denoising results of the four algorithms. (<b>a</b>) WT denoising algorithm. (<b>b</b>) EMD-WT denoising algorithm. (<b>c</b>) VMD-WT denoising algorithm. (<b>d</b>) ISGMD-WT denoising algorithm.</p>
Full article ">Figure 5
<p>The original signal and the mixed signals with different noise decibels.</p>
Full article ">Figure 6
<p>Denoising effect of four algorithms with 0 db noise decibel. (<b>a</b>) WT. (<b>b</b>) EMD-WT. (<b>c</b>) VMD-WT. (<b>d</b>) ISGMD-WT.</p>
Full article ">Figure 6 Cont.
<p>Denoising effect of four algorithms with 0 db noise decibel. (<b>a</b>) WT. (<b>b</b>) EMD-WT. (<b>c</b>) VMD-WT. (<b>d</b>) ISGMD-WT.</p>
Full article ">Figure 7
<p>Denoising effect of four algorithms with 5 db noise decibel. (<b>a</b>) WT. (<b>b</b>) EMD-WT. (<b>c</b>) VMD-WT. (<b>d</b>) ISGMD-WT.</p>
Full article ">Figure 8
<p>Denoising effect of four algorithms with 10 db noise decibel. (<b>a</b>) WT. (<b>b</b>) EMD-WT. (<b>c</b>) VMD-WT. (<b>d</b>) ISGMD-WT.</p>
Full article ">Figure 9
<p>Hydrophone experiment. (<b>a</b>) The Olympus-v389-su hydrophone. (<b>b</b>) Experimental platform.</p>
Full article ">Figure 10
<p>The time-domain signal received by the hydrophone and the spectrogram of signal. (<b>a</b>) Time-domain signal. (<b>b</b>) The spectrogram of signal.</p>
Full article ">Figure 11
<p>The clusters generated by spectral clustering.</p>
Full article ">Figure 12
<p>Denoised signals generated by the four algorithms.</p>
Full article ">Figure 13
<p>The spectrogram of denoised signals generated by the four algorithms. (<b>a</b>) WT. (<b>b</b>) EMD-WT. (<b>c</b>) VMD-WT. (<b>d</b>) ISGMD-WT.</p>
Full article ">
15 pages, 4811 KiB  
Article
Stability Analysis of Metal Active-Gas Welding Short-Circuiting Transfer Based on Input Pulsating Energy
by Xiaoqing Lv, Quanjun He and Lianyong Xu
Materials 2024, 17(2), 274; https://doi.org/10.3390/ma17020274 - 5 Jan 2024
Viewed by 1130
Abstract
In this study, a platform for a welding experiment, used to collect input and output electrical signals, was constructed, and the algorithm for the input pulsating energy interpolation line (IPEI) was given. Experiments with MAG surface straight line welding were conducted at various [...] Read more.
In this study, a platform for a welding experiment, used to collect input and output electrical signals, was constructed, and the algorithm for the input pulsating energy interpolation line (IPEI) was given. Experiments with MAG surface straight line welding were conducted at various voltages. Analysis of the IPEI in relation to the welding current was performed while combining real-world welding occurrences with high-speed camera images of droplet transfer. It was established that the IPEI can be employed as a characteristic parameter to assess the stability of the short-circuiting transfer process in MAG welding. The three criteria for assessing the stability were the spectrum, approximation entropy, and coefficient of variation. A comparative analysis was conducted on each of these approaches. It was determined that the most effective technique is approximation entropy. The approximation entropy of the welding current and IPEI are also highly consistent, with a correlation coefficient as high as 0.9889. Full article
(This article belongs to the Special Issue Research on Advanced Welding Techniques)
Show Figures

Figure 1

Figure 1
<p>Schematic diagram of the experimental platform.</p>
Full article ">Figure 2
<p>Flow diagram for the synchronizing high-speed camera and electrical signal acquisition.</p>
Full article ">Figure 3
<p>Three-phase full-bridge uncontrolled rectifier circuit.</p>
Full article ">Figure 4
<p>Input line voltage of the welding machine.</p>
Full article ">Figure 5
<p>Input line current of welding machine.</p>
Full article ">Figure 6
<p>Instantaneous input power and welding current.</p>
Full article ">Figure 7
<p>Input pulsating energy and welding current.</p>
Full article ">Figure 8
<p>IPEI and welding current.</p>
Full article ">Figure 9
<p>Welding current and IPEI waveforms, high-speed camera photos, and weld seam formation at different given voltages (<b>a</b>: <b>a1</b>–<b>a3</b>) 15 V, (<b>b</b>: <b>b1</b>–<b>b3</b>) 19 V, (<b>c</b>: <b>c1</b>–<b>c3</b>) 23 V, (<b>d</b>: <b>d1</b>–<b>d3</b>) 27 V.</p>
Full article ">Figure 10
<p>Spectra of welding current and IPEI at different given voltages. (<b>a</b>) 15 V, (<b>b</b>) 19 V, (<b>c</b>) 23 V, (<b>d</b>) 27 V.</p>
Full article ">Figure 11
<p>The comparison of the CVs for IPEI and welding current.</p>
Full article ">Figure 12
<p>The comparison of the ApEns of IPEI and welding current.</p>
Full article ">
12 pages, 442 KiB  
Article
The Spectrum of Low-pT J/ψ in Heavy-Ion Collisions in a Statistical Two-Body Fractal Model
by Huiqiang Ding, Luan Cheng, Tingting Dai, Enke Wang and Wei-Ning Zhang
Entropy 2023, 25(12), 1655; https://doi.org/10.3390/e25121655 - 13 Dec 2023
Viewed by 1166
Abstract
We establish a statistical two-body fractal (STF) model to study the spectrum of J/ψ. J/ψ serves as a reliable probe in heavy-ion collisions. The distribution of J/ψ in hadron gas is influenced by flow, quantum and [...] Read more.
We establish a statistical two-body fractal (STF) model to study the spectrum of J/ψ. J/ψ serves as a reliable probe in heavy-ion collisions. The distribution of J/ψ in hadron gas is influenced by flow, quantum and strong interaction effects. Previous models have predominantly focused on one or two of these effects while neglecting the others, resulting in the inclusion of unconsidered effects in the fitted parameters. Here, we study the issue from a new point of view by analyzing the fact that all three effects induce a self-similarity structure, involving a J/ψ-π two-meson state and a J/ψ, π two-quark state, respectively. We introduce modification factor qTBS and q2 into the probability and entropy of charmonium. qTBS denotes the modification of self-similarity on J/ψ, q2 denotes that of self-similarity and strong interaction between c and c¯ on quarks. By solving the probability and entropy equations, we derive the values of qTBS and q2 at various collision energies and centralities. Substituting the value of qTBS into distribution function, we successfully obtain the transverse momentum spectrum of low-pT J/ψ, which demonstrates good agreement with experimental data. The STF model can be employed to investigate other mesons and resonance states. Full article
(This article belongs to the Section Statistical Physics)
Show Figures

Figure 1

Figure 1
<p>The self-similarity structure of <span class="html-italic">c</span> and <math display="inline"><semantics> <mover accent="true"> <mi>c</mi> <mo>¯</mo> </mover> </semantics></math> in the hadron gas near to the critical temperature. (<b>a</b>) <math display="inline"><semantics> <mrow> <mi>J</mi> <mo>/</mo> <mi>ψ</mi> </mrow> </semantics></math> in hadron gas from the quark aspect; (<b>b</b>) <math display="inline"><semantics> <mrow> <mi>J</mi> <mo>/</mo> <mi>ψ</mi> </mrow> </semantics></math> in hadron gas from the meson aspect; (<b>c</b>) <math display="inline"><semantics> <mrow> <mi>J</mi> <mo>/</mo> <mi>ψ</mi> </mrow> </semantics></math>-<math display="inline"><semantics> <mi>π</mi> </semantics></math> two-body self-similarity structure from the partial picture and the whole picture.</p>
Full article ">Figure 2
<p>Influencing factor <math display="inline"><semantics> <msub> <mi>q</mi> <mrow> <mi>T</mi> <mi>B</mi> <mi>S</mi> </mrow> </msub> </semantics></math> at different fixed temperature swith <math display="inline"><semantics> <mrow> <msub> <mi>r</mi> <mn>0</mn> </msub> <mo>=</mo> <mn>3.48</mn> <mo>,</mo> <mn>3.56</mn> <mo>,</mo> <mn>3.63</mn> <mspace width="0.166667em"/> <mi>fm</mi> </mrow> </semantics></math>.</p>
Full article ">Figure 3
<p>Transverse momentum spectra of <math display="inline"><semantics> <mrow> <mi>J</mi> <mo>/</mo> <mi>ψ</mi> </mrow> </semantics></math> in Au–Au collisions at <math display="inline"><semantics> <msqrt> <msub> <mi>s</mi> <mi>NN</mi> </msub> </msqrt> </semantics></math> = 39 GeV for different centrality classes in mid-rapidity region <math display="inline"><semantics> <mrow> <mo stretchy="false">|</mo> <mi>y</mi> <mo stretchy="false">|</mo> <mo>&lt;</mo> <mn>1.0</mn> </mrow> </semantics></math>. The experimental data are taken from STAR [<a href="#B60-entropy-25-01655" class="html-bibr">60</a>].</p>
Full article ">Figure 4
<p>Transverse momentum spectra of <math display="inline"><semantics> <mrow> <mi>J</mi> <mo>/</mo> <mi>ψ</mi> </mrow> </semantics></math> in Au–Au collisions at <math display="inline"><semantics> <msqrt> <msub> <mi>s</mi> <mi>NN</mi> </msub> </msqrt> </semantics></math> = 62.4 GeV for different centrality classes in mid-rapidity region <math display="inline"><semantics> <mrow> <mo stretchy="false">|</mo> <mi>y</mi> <mo stretchy="false">|</mo> <mo>&lt;</mo> <mn>1.0</mn> </mrow> </semantics></math>. The experimental data are taken from STAR [<a href="#B60-entropy-25-01655" class="html-bibr">60</a>].</p>
Full article ">Figure 5
<p>Transverse momentum spectra of <math display="inline"><semantics> <mrow> <mi>J</mi> <mo>/</mo> <mi>ψ</mi> </mrow> </semantics></math> in Au–Au collisions at <math display="inline"><semantics> <msqrt> <msub> <mi>s</mi> <mi>NN</mi> </msub> </msqrt> </semantics></math> = 200 GeV for different centrality classes in mid-rapidity region <math display="inline"><semantics> <mrow> <mo stretchy="false">|</mo> <mi>y</mi> <mo stretchy="false">|</mo> <mo>&lt;</mo> <mn>1.0</mn> </mrow> </semantics></math>. The experimental data are taken from STAR [<a href="#B61-entropy-25-01655" class="html-bibr">61</a>].</p>
Full article ">
23 pages, 7443 KiB  
Article
A Technique for Bearing Fault Diagnosis Using Novel Wavelet Packet Transform-Based Signal Representation and Informative Factor LDA
by Andrei S. Maliuk, Zahoor Ahmad and Jong-Myon Kim
Machines 2023, 11(12), 1080; https://doi.org/10.3390/machines11121080 - 11 Dec 2023
Cited by 3 | Viewed by 2086
Abstract
This paper proposes a new method for bearing fault diagnosis using wavelet packet transform (WPT)-based signal representation and informative factor linear discriminant analysis (IF-LDA). Time–frequency domain approaches for analyzing bearing vibration signals have gained wide acceptance due to their effectiveness in extracting information [...] Read more.
This paper proposes a new method for bearing fault diagnosis using wavelet packet transform (WPT)-based signal representation and informative factor linear discriminant analysis (IF-LDA). Time–frequency domain approaches for analyzing bearing vibration signals have gained wide acceptance due to their effectiveness in extracting information related to bearing health. WPT is a prominent method in this category, offering a balanced approach between short-time Fourier transform and empirical mode decomposition. However, the existing methods for bearing fault diagnosis often overlook the limitations of WPT regarding its dependence on the mother wavelet parameters for feature extraction. This work addresses this issue by introducing a novel signal representation method that employs WPT with a new rule for selecting the mother wavelet based on the power spectrum energy-to-entropy ratio of the reconstructed coefficients and a combination of the nodes from different WPT trees. Furthermore, an IF-LDA feature preprocessing technique is proposed, resulting in a highly sensitive set of features for bearing condition assessment. The k-nearest neighbors algorithm is employed as the classifier, and the proposed method is evaluated using datasets from Paderborn and Case Western Reserve universities. The performance of the proposed method demonstrates its effectiveness in bearing fault diagnosis, surpassing existing techniques in terms of fault identification and diagnosis performance. Full article
(This article belongs to the Special Issue New Advances in Rotating Machinery)
Show Figures

Figure 1

Figure 1
<p>Paderborn University testbed.</p>
Full article ">Figure 2
<p>Time- and frequency-domain plots illustrative of all types of faults in the PUA dataset.</p>
Full article ">Figure 3
<p>Time- and frequency-domain plots illustrative of all types of faults in the PUR dataset.</p>
Full article ">Figure 4
<p>Case Western Reserve University testbed.</p>
Full article ">Figure 5
<p>Time- and frequency-domain plots illustrative of all types of faults in the CWRU dataset.</p>
Full article ">Figure 6
<p>The scheme of the wavelet packet tree.</p>
Full article ">Figure 7
<p>Workflow of the proposed method.</p>
Full article ">Figure 8
<p>Construction flow of the novel WPT-based representation.</p>
Full article ">Figure 9
<p>Three-dimensional IF-LDA feature space representations obtained from the proposed method.</p>
Full article ">Figure 10
<p>True positive rates for each bearing fault acquired as a result of testing the proposed and comparison methods on three datasets. The columns in black, orange, grey, and yellow stand for the bearing fault class. Each set of columns has a caption that indicates the comparison method to which it belongs.</p>
Full article ">Figure 11
<p>Averaged performance metrics for the proposed and comparison methods obtained from testing on three datasets. The columns in black, orange, grey, and yellow stand for the bearing fault class. Each set of columns has a caption that indicates the comparison method to which it belongs.</p>
Full article ">
Back to TopTop