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Keywords = Hölder space

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14 pages, 3752 KiB  
Article
Investigation of Pore Size on the Hydrogen Evolution Reaction of 316L Stainless Steel Porous Electrodes
by Victor Manuel Solorio, Luis Olmos, Melina Velasco-Plascencia, Héctor J. Vergara-Hernández, Julio C. Villalobos, Mario Misael Machado López and Juan Manuel Salgado López
Catalysts 2025, 15(1), 38; https://doi.org/10.3390/catal15010038 - 3 Jan 2025
Viewed by 470
Abstract
This work aims to analyze the effect of pore size on the catalytic reaction of 316L stainless steel electrodes. Porous compacts were fabricated using the space holder technique and sintering at low temperatures. The fabricated porous compacts were characterized using computed tomography and [...] Read more.
This work aims to analyze the effect of pore size on the catalytic reaction of 316L stainless steel electrodes. Porous compacts were fabricated using the space holder technique and sintering at low temperatures. The fabricated porous compacts were characterized using computed tomography and the hydrogen evolution reaction was evaluated under 0.5 M and 1.5 M NaOH. Results indicate that porosity is well controlled by the pore formers, which allows different pore size distributions of pores with similar relative density values to be obtained. The pores are fully interconnected, allowing the passing of fluid throughout the compacts. Permeability is sensitive to the pore size, increasing as the pore size does. The catalytic activity of hydrogen evolution reaction HER is improved as the pore volume and pore size increase concerning the compact fabricated without pore formers. The compact that showed higher Cdl and Rf values was fabricated with S100 pore formers, which means a higher active area that favors the HER. It can be concluded that porosity enhances HER reactivity. However, larger pores are not beneficial due to a more significant permeability value. Full article
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<p>Shrinkage as a function of time and temperature during sintering samples without and with three different particle size distributions of pore formers powders.</p>
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<p>Sintered density as a function of the particle size distribution of pore formers.</p>
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<p>2D virtual slices and 3D rendering of a REV extracted from the center of WS samples fabricated without pore formers (<b>a</b>,<b>e</b>), and with 30% of pore formers with different particle size distributions; (<b>b</b>,<b>f</b>) S100, (<b>c</b>,<b>g</b>) S200, (<b>d</b>,<b>h</b>) S300, respectively. The white rectangle indicates where the inner volume was extracted to make the 3D rendering.</p>
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<p>2D virtual slices of the sample without pore formers showing the image processing, (<b>a</b>) initial, binary images of (<b>b</b>) 316L particles, and (<b>c</b>) pores.</p>
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<p>Pore size distributions of samples without and with pore formers of different sizes.</p>
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<p>3D rendering of the porosity after sintering of samples (<b>a</b>) WS and (<b>b</b>) S300 particle; distribution and streamlines for the flow of water through pores in the vertical direction for both samples (<b>c</b>) without and (<b>d</b>) with pore formers particles. The color of the streamlines indicates the flow velocity, being the red the fastest and blue slowest.</p>
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<p>Permeability estimated from numerical simulations as a function of (<b>a</b>) specific surface and (<b>b</b>) median pore size.</p>
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<p>HER current density of porous stainless steel as a function of particle size, evaluated with (<b>a</b>) 0.5 M NaOH and (<b>b</b>) 1.5 M NaOH.</p>
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<p>EIS at 0.5 M NaOH, (<b>a</b>) Nyquist diagram, (<b>b</b>) Bode diagram—impedance magnitude and (<b>c</b>) Bode diagram—phase angle; EIS at 1.5 M NaOH, (<b>d</b>) Nyquist diagram, (<b>e</b>) Bode diagram—impedance magnitude and (<b>f</b>) Bode diagram—phase angle.</p>
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<p>Electrochemical equivalent circuit used by modeling <span class="html-italic">R<sub>CT</sub></span> and <span class="html-italic">C<sub>dl</sub></span> in 316L stainless steel in the different sintering conditions.</p>
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15 pages, 8804 KiB  
Article
Development of Short-Titanium-Fiber-Reinforced Porous Titanium as Biometal for Implants
by So Shimizu, Tomoyuki Fujii and Yoshinobu Shimamura
J. Compos. Sci. 2025, 9(1), 10; https://doi.org/10.3390/jcs9010010 - 2 Jan 2025
Viewed by 339
Abstract
Biometals used for the replacement of damaged bones are required to have a Young’s modulus comparable with that of the surrounding bones, in addition to having no toxicity, high corrosion resistance, and high strength. The Young’s modulus of natural bones is much lower [...] Read more.
Biometals used for the replacement of damaged bones are required to have a Young’s modulus comparable with that of the surrounding bones, in addition to having no toxicity, high corrosion resistance, and high strength. The Young’s modulus of natural bones is much lower than those of common biometals. Porous biometals have been widely studied to achieve a lower Young’s modulus. However, these materials commonly exhibit low strength because the pores tend to behave as microscopic defects. In this study, porous titanium, a promising biometal, was reinforced with short titanium fibers. The porous structure and fiber reinforcement provided a low Young’s modulus and relatively high strength, respectively. The short-titanium-fiber-reinforced porous titanium was fabricated using the space holder method with spark plasma sintering. The porosity of the matrix (uniform porous titanium), volume fraction of the fibers, and aspect ratio were set to 60%, 30%, and 8 to 64, respectively. A bending test revealed that the Young’s modulus was low and almost constant, irrespective of the aspect ratio, and that the strength increased with an increased aspect ratio. A high strength, which is difficult to obtain with uniform porous titanium, and a low Young’s modulus were achieved by applying fiber reinforcement. The results demonstrate that short-titanium-fiber-reinforced porous titanium is a candidate biometal for the replacement of damaged bones. Full article
(This article belongs to the Special Issue Feature Papers in Journal of Composites Science in 2024)
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<p>SEM images of (<b>a</b>) Ti powder, (<b>b</b>) NaCl powder, and (<b>c</b>) Ti fiber.</p>
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<p>Typical changes in the current and temperature during sintering. These changes were measured when the specimen that included Ti fibers with an aspect ratio of 32 was sintered, and the same trend was observed for other specimens.</p>
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<p>Schematic diagrams of (<b>a</b>) transverse (top and bottom surfaces) and (<b>b</b>) longitudinal sections of short-Ti-fiber-reinforced porous Ti. Each black ellipse denotes the cross-section of a Ti fiber.</p>
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<p>Dimensions of a three-point bending test specimen. (<b>a</b>) Dimensions of the specimen and loading conditions and (<b>b</b>) positions of the load line and fracture plane. Fracture may occur on the tensile side at a distance of <span class="html-italic">x</span> from the center (the load line).</p>
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<p>Porosity of short-Ti-fiber-reinforced porous Ti as function of aspect ratio of Ti fibers.</p>
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<p>Microstructure of the short-Ti-fiber-reinforced porous Ti with an aspect ratio of 8. (<b>a</b>) Top surface (transverse section) and (<b>b</b>) longitudinal section. The direction of the pulse current during the SPS is shown.</p>
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<p>Microstructure of the short-Ti-fiber-reinforced porous Ti with an aspect ratio of 64. (<b>a</b>) Top surface (transverse section) and (<b>b</b>) longitudinal section. The direction of the pulse current during the SPS is shown.</p>
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<p>Distributions of the short Ti fibers in the (<b>a</b>) in-plane and (<b>b</b>) out-of-plane directions. The angles were measured in the range of −90° to +90°. It is not necessary to distinguish between positive and negative values to show the deviation from the reference line. Therefore, the angles are shown as absolute values.</p>
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<p>Typical load–displacement curves in three-point bending tests.</p>
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<p>Mechanical properties of short-Ti-fiber-reinforced porous Ti. (<b>a</b>) Young’s modulus and (<b>b</b>) bending strength as function of Ti fiber aspect ratio.</p>
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<p>SEM images of the fracture morphology of porous Ti. The arrows denote the load line shown in <a href="#jcs-09-00010-f004" class="html-fig">Figure 4</a>. (<b>a</b>) SEM image of the bottom surface in the vicinity of the fracture site of the porous Ti with no reinforcement. SEM images of the bottom surfaces at the fracture sites of the porous Ti with aspect ratios of (<b>b</b>) 8 and (<b>c</b>) 64. (<b>d</b>–<b>f</b>) show magnified SEM images corresponding to (<b>a</b>–<b>c</b>), respectively. Microscopic fracture progressed by avoiding the Ti fibers, as shown by red circles in (<b>e</b>), when the aspect ratio was low. Fracture progressed via fiber breakage, as shown by red circles in (<b>f</b>), when the aspect ratio was high. The fracture in the matrix of the fiber-reinforced porous Ti was almost the same as that in the uniform porous Ti shown in (<b>d</b>).</p>
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<p>Fracture surfaces of the porous Ti. (<b>a</b>,<b>b</b>) show both fracture surfaces of the uniform porous Ti. (<b>c</b>,<b>d</b>) and (<b>e</b>,<b>f</b>) show both fracture surfaces of the porous Ti with aspect ratios of 8 and 64, respectively. The solid and dashed circles show the fiber pull-out and fiber breakage, respectively. More fibers tended to break as the aspect ratio increased.</p>
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13 pages, 258 KiB  
Article
Analyzing Uniqueness of Solutions in Nonlinear Fractional Differential Equations with Discontinuities Using Lebesgue Spaces
by Farva Hafeez, Mdi Begum Jeelani and Nouf Abdulrahman Alqahtani
Axioms 2025, 14(1), 26; https://doi.org/10.3390/axioms14010026 - 31 Dec 2024
Viewed by 286
Abstract
We explore the existence and uniqueness of solutions to nonlinear fractional differential equations (FDEs), defined in the sense of RL-fractional derivatives of order η(1,2). The nonlinear term is assumed to have a discontinuity at zero. By [...] Read more.
We explore the existence and uniqueness of solutions to nonlinear fractional differential equations (FDEs), defined in the sense of RL-fractional derivatives of order η(1,2). The nonlinear term is assumed to have a discontinuity at zero. By employing techniques from Lebesgue spaces, including Holder’s inequality, we establish uniqueness theorems for this problem, analogous to Nagumo, Krasnoselskii–Krein, and Osgood-type results. These findings provide a fundamental framework for understanding the properties of solutions to nonlinear FDEs with discontinuous nonlinearities. Full article
(This article belongs to the Special Issue Fractional Calculus—Theory and Applications, 3rd Edition)
29 pages, 401 KiB  
Article
Equivalence Between Fractional Differential Problems and Their Corresponding Integral Forms with the Pettis Integral
by Mieczysław Cichoń, Wafa Shammakh, Kinga Cichoń and Hussein A. H. Salem
Mathematics 2024, 12(23), 3642; https://doi.org/10.3390/math12233642 - 21 Nov 2024
Viewed by 442
Abstract
The problem of equivalence between differential and integral problems is absolutely crucial when applying solution methods based on operators and their properties in function spaces. In this paper, we complement the solution of this important problem by considering the case of general derivatives [...] Read more.
The problem of equivalence between differential and integral problems is absolutely crucial when applying solution methods based on operators and their properties in function spaces. In this paper, we complement the solution of this important problem by considering the case of general derivatives and integrals of fractional order for vector functions for weak topology. Even if a Caputo differential fractional order problem has a right-hand side that is weakly continuous, the equivalence between the differential and integral forms may be affected. In this paper, we present a complete solution to this problem using fractional order Pettis integrals and suitably defined pseudo-derivatives, taking care to construct appropriate Hölder-type spaces on which the operators under study are mutually inverse. In this paper, we prove, in a number of cases, the equivalence of differential and integral problems in Hölder spaces and, by means of appropriate counter-examples, investigate cases where this property of the problems is absent. Full article
(This article belongs to the Special Issue Fractional Calculus and Mathematical Applications, 2nd Edition)
13 pages, 799 KiB  
Article
Integral Operators in b-Metric and Generalized b-Metric Spaces and Boundary Value Problems
by Christopher Middlebrook and Wenying Feng
Fractal Fract. 2024, 8(11), 674; https://doi.org/10.3390/fractalfract8110674 - 19 Nov 2024
Viewed by 630
Abstract
We study fixed-point theorems of contractive mappings in b-metric space, cone b-metric space, and the newly introduced extended b-metric space. To generalize an existence and uniqueness result for the so-called Φs functions in the b-metric space to the extended b-metric space and [...] Read more.
We study fixed-point theorems of contractive mappings in b-metric space, cone b-metric space, and the newly introduced extended b-metric space. To generalize an existence and uniqueness result for the so-called Φs functions in the b-metric space to the extended b-metric space and the cone b-metric space, we introduce the class of ΦM functions and apply the Hölder continuous condition in the extended b-metric space. The obtained results are applied to prove the existence and uniqueness of solutions and positive solutions for nonlinear integral equations and fractional boundary value problems. Examples and numerical simulation are given to illustrate the applications. Full article
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<p><math display="inline"><semantics> <mrow> <mi>λ</mi> <mo>=</mo> <mn>2.9</mn> <mo>,</mo> <mi>α</mi> <mo>=</mo> <mn>2.4</mn> <mo>,</mo> <mi>ε</mi> <mo>=</mo> <mn>0.01</mn> </mrow> </semantics></math>.</p>
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<p><math display="inline"><semantics> <mrow> <mi>λ</mi> <mo>=</mo> <mn>2.9</mn> <mo>,</mo> <mi>α</mi> <mo>=</mo> <mn>2.8</mn> <mo>,</mo> <mi>ε</mi> <mo>=</mo> <mn>0.01</mn> </mrow> </semantics></math>.</p>
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33 pages, 394 KiB  
Article
On the Problem of the Uniqueness of Fixed Points and Solutions for Quadratic Fractional-Integral Equations on Banach Algebras
by Kinga Cichoń, Mieczysław Cichoń and Maciej Ciesielski
Symmetry 2024, 16(11), 1535; https://doi.org/10.3390/sym16111535 - 16 Nov 2024
Viewed by 553
Abstract
In this paper, we study the problem of the uniqueness of fixed points for operators defined on subspaces of the space of continuous functions C[a,b] equipped with norms stronger than the supremum norm. We are particularly interested in [...] Read more.
In this paper, we study the problem of the uniqueness of fixed points for operators defined on subspaces of the space of continuous functions C[a,b] equipped with norms stronger than the supremum norm. We are particularly interested in Hölder spaces since they are natural ranges of integral operators of fractional order. Our goal is to preserve the expected regularity of the fixed points (solutions of the equations) when investigating their uniqueness, without assuming a contraction condition on the space under study. We claim some symmetry between the case of the obtained results and the case of the classical Banach fixed-point theorem in such spaces, even for operators which are not necessarily contractions in the sense of the norm of these subspaces. This result is of particular interest for the study of quadratic integral equations, and as an application example we prove the uniqueness theorem for such a kind equations with general fractional order integral operators, which are not necessarily contractions, in a suitably constructed generalized Hölder space. Full article
(This article belongs to the Special Issue New Trends in Fixed Point Theory with Emphasis on Symmetry)
25 pages, 13336 KiB  
Article
Synthesis and Characterization of Ti-13Ta-6Sn Foams Produced Using Mechanical Alloying, the Space Holder Method and Plasma-Assisted Sintering
by Francisco Cavilha Neto, Vagner Kretiska Medeiros, Vicente Salinas-Barrera, Edgar Pio, Claudio Aguilar, Bruno Borges Ramos, Aloísio Nelmo Klein, Bruno Henriques and Cristiano Binder
Metals 2024, 14(10), 1145; https://doi.org/10.3390/met14101145 - 8 Oct 2024
Viewed by 1170
Abstract
Highly porous titanium foams are great candidates for replacing bone structures with a low elastic modulus owing to their ability to avoid the stress shielding effect. However, the production of highly porous foams (>70 vol.%) with well-distributed, stable, and predictable porous architectures using [...] Read more.
Highly porous titanium foams are great candidates for replacing bone structures with a low elastic modulus owing to their ability to avoid the stress shielding effect. However, the production of highly porous foams (>70 vol.%) with well-distributed, stable, and predictable porous architectures using powder compaction and space holders is challenging. In this study, pure titanium powder and mechanically alloyed Ti-13Ta-6Sn were mixed with 50, 70, and 80 vol.% KCl powders as a space holder, cold-compacted, and sintered in a plasma-assisted sintering reactor to produce highly porous foams. The space holder was completely removed using heat and plasma species collisions prior to sintering. A Ti-13Ta-6Sn alloy powder with α, β, and metastable FCC-γ phases was synthesized. The characteristics of the alloyed powder, mixing step, and the resulting sintered samples were compared to those of CP-Ti. After sintering, the alloy exhibited α and β phases and a reduced elastic modulus. Foams with an elastic modulus in the range of the cortical and trabecular bones were obtained. The results showed the effects of the space holder volume fractions on the volume fraction, size, distribution, interconnectivity, and shape of the pores. The Ti-13Ta-6Sn foams exhibited a uniform open-celled porous architecture, lower elastic modulus, higher yield strength, and higher passivation resistance than CP-Ti. Ti-13Ta-6Sn exhibited a nontoxic effect for the mouse fibroblast cell line. Full article
(This article belongs to the Special Issue Progress in Biomedical Metallic Materials and Surfaces)
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Figure 1
<p>SEM images of the starting powders: (<b>a</b>) CP-Ti at 500×, (<b>b</b>) Ti-13Ta-6Sn at 30,000×, and (<b>c</b>) KCl particles at 500×.</p>
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<p>X-ray diffraction pattern of milled Ti-13Ta-6Sn powder with Rietveld refinement results.</p>
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<p>Relative density variation as a function of compaction pressure for powders with and without space holders (SH).</p>
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<p>KCl particles mixed with (<b>a</b>) CP and (<b>b</b>) Ti-13Ta-6Sn powders, and (<b>c</b>) KCl size and distribution analysis by laser diffraction.</p>
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<p>Transversal cross-sections of sintered dense (<b>a</b>) CP-Ti and (<b>b</b>) Ti-13Ta-6Sn.</p>
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<p>Plasma-assisted sintered samples of CP-Ti (<b>a</b>) dense, (<b>b</b>) 50% SH, (<b>c</b>) 70% SH, and (<b>d</b>) 80% SH and Ti-13Ta-6Sn (<b>e</b>) dense, (<b>f</b>) 50% SH, (<b>g</b>) 70% SH, and (<b>h</b>) 80% SH. Images were obtained using a digital camera.</p>
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<p>Foam cross-sections captured by SEM of CP-Ti with (<b>a</b>) 50%, (<b>b</b>) 70%, and (<b>c</b>) 80% space holders and Ti-13Ta-6Sn with (<b>d</b>) 50%, (<b>e</b>) 70%, and (<b>f</b>) 80% space holders.</p>
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<p>Foam cross-sections captured by SEM of CP-Ti with (<b>a</b>) 50%, (<b>b</b>) 70%, and (<b>c</b>) 80% space holders and Ti-13Ta-6Sn with (<b>d</b>) 50%, (<b>e</b>) 70%, and (<b>f</b>) 80% space holders.</p>
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<p>Pore SEM-EDS analysis of porous (<b>a</b>) CP-Ti and (<b>b</b>) Ti-13Ta-6Sn.</p>
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<p>Effect of space holder volume fraction on porosity percentage of CP-Ti and Ti-13Ta-6Sn alloy.</p>
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<p>Reconstructed 3D images of (<b>a</b>) CP-Ti 50%, (<b>b</b>) CP-Ti 70%, (<b>c</b>) CP-Ti 80%, (<b>d</b>) Ti-13Ta-6Sn 50%, (<b>e</b>) Ti-13Ta-6Sn 70%, and (<b>f</b>) Ti-13Ta-6Sn 80% obtained using X-ray microcomputed tomography.</p>
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<p>Pore volume fraction per slice of (<b>a</b>) CP-Ti and (<b>b</b>) Ti-13Ta-6Sn alloys.</p>
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<p>Pore size distributions of (<b>a</b>) CP-Ti and (<b>b</b>) Ti-13Ta-6Sn foams produced with 50, 70, and 80% of SH in volume. Dashed lines indicate total average pore size for each added SH volume fraction.</p>
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<p>Sphericity distributions of (<b>a</b>) CP-Ti and (<b>b</b>) Ti-13Ta-6Sn alloys.</p>
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<p>Measured engineering stress–strain curves obtained by compressive tests of (<b>a</b>) all samples, (<b>b</b>) all foams, (<b>c</b>) CP-Ti foams, and (<b>d</b>) Ti-13Ta-6Sn foams.</p>
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<p>Measured dynamic elastic moduli of dense CP-Ti and Ti-13Ta-6Sn with standard deviation.</p>
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<p>Measured dynamic elastic moduli of porous CP-Ti and Ti-13Ta-6Sn.</p>
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<p>Typical potentiodynamic polarization curves obtained from the analyzed samples.</p>
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<p>Qualitative cytotoxicity analysis of dense Ti-13Ta-6Sn measured each 12 h for a total analysis of 48 h following ISO 10993-5. Black squares indicate the reactivity level at each measurement.</p>
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15 pages, 313 KiB  
Article
Variable Lebesgue Space over Weighted Homogeneous Tree
by Yuxun Zhang and Jiang Zhou
Symmetry 2024, 16(10), 1283; https://doi.org/10.3390/sym16101283 - 30 Sep 2024
Viewed by 809
Abstract
An infinite homogeneous tree is a special type of graph that has a completely symmetrical structure in all directions. For an infinite homogeneous tree T=(V,E) with the natural distance d defined on graphs and a weighted measure [...] Read more.
An infinite homogeneous tree is a special type of graph that has a completely symmetrical structure in all directions. For an infinite homogeneous tree T=(V,E) with the natural distance d defined on graphs and a weighted measure μ of exponential growth, the authors introduce the variable Lebesgue space Lp(·)(μ) over (V,d,μ) and investigate it under the global Hölder continuity condition for p(·). As an application, the strong and weak boundedness of the maximal operator relevant to admissible trapezoids on Lp(·)(μ) is obtained, and an unbounded example is presented. Full article
(This article belongs to the Special Issue Symmetry in Functional Analysis and Operator Theory)
14 pages, 3505 KiB  
Article
Enhancing Capillary Pressure of Porous Aluminum Wicks by Controlling Bi-Porous Structure Using Different-Sized NaCl Space Holders
by Hongfei Shen, Asuka Suzuki, Naoki Takata and Makoto Kobashi
Materials 2024, 17(19), 4729; https://doi.org/10.3390/ma17194729 - 26 Sep 2024
Viewed by 572
Abstract
Capillary pressure and permeability of porous media are important for heat transfer devices, including loop heat pipes. In general, smaller pore sizes enhance capillary pressure but decrease permeability. Introducing a bi-porous structure is promising for solving this trade-off relation. In this study, the [...] Read more.
Capillary pressure and permeability of porous media are important for heat transfer devices, including loop heat pipes. In general, smaller pore sizes enhance capillary pressure but decrease permeability. Introducing a bi-porous structure is promising for solving this trade-off relation. In this study, the bi-porous aluminum was fabricated by the space holder method using two different-sized NaCl particles (approximately 400 and 40 μm). The capillary pressure and permeability of the bi-porous Al were evaluated and compared with those of mono-porous Al fabricated by the space holder method. Increasing the porosity of the mono-porous Al improved the permeability but reduced the capillary pressure because of better-connected pores and increased effective pore size. The fraction of large and small pores in the bi-porous Al was successfully controlled under a constant porosity of 70%. The capillary pressure of the bi-porous Al with 40% large and 30% small pores was higher than the mono-porous Al with 70% porosity without sacrificing the permeability. However, the bi-porous Al with other fractions of large and small pores did not exhibit properties superior to the mono-porous Al. Thus, accurately controlling the fractions of large and small pores is required to enhance the capillary performance by introducing the bi-porous structure. Full article
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<p>SEM images of raw materials and fabrication process of bi-porous Al using space holder method.</p>
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<p>Schematic illustration of setup for measuring the capillary performance of porous samples in this study [<a href="#B27-materials-17-04729" class="html-bibr">27</a>].</p>
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<p>Representative SEM images of mono-porous Al: (<b>a</b>) S50, (<b>b</b>) S60, and (<b>c</b>) S70.</p>
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<p>(<b>a</b>) Time evolution of the capillary rising height of mono-porous Al. (<b>b</b>) Relationship between capillary rising rate and reciprocal height.</p>
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<p>SEM images of bi-porous Al: (<b>a</b>) L60S10, (<b>b</b>) L50S20, (<b>c</b>) L40S30, and (<b>d</b>) L30S40.</p>
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<p>(<b>a</b>) Time evolution of the capillary rising height of bi-porous Al. (<b>b</b>) Relationship between capillary rising rate and reciprocal height.</p>
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<p>Change in (<b>a</b>) permeability, capillary pressure, and (<b>b</b>) their product with the volume fraction of small NaCl particles.</p>
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<p>Plot of permeability and capillary pressure of mono-porous and bi-porous Al.</p>
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<p>Changes in the average sizes of large, small, and overall pores as a function of the volume fraction of small NaCl particles. The flow channel size calculated from Equation (1) is also shown in this figure.</p>
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<p>Hypothetical schematic illustration of capillary rising behaviors in (<b>a</b>) L60S10, L50S20, (<b>b</b>) L40S30, and (<b>c</b>) L30S40. The complex porous structures are simplified into straight channel models in (<b>d</b>–<b>f</b>).</p>
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25 pages, 3450 KiB  
Article
Shamans and “Dark Agencies”: War, Magical Parasitism, and Re-Enchanted Spirits in Siberia
by Konstantinos Zorbas
Religions 2024, 15(10), 1150; https://doi.org/10.3390/rel15101150 - 24 Sep 2024
Viewed by 1072
Abstract
Alleged practices of magical assault and vampirism are a recurrent feature of popular explanations of misfortune in Tuva, South Siberia. Based on a field study of healing practices in an “Association of Shamans”, this article analyses rituals of redressing curse afflictions in the [...] Read more.
Alleged practices of magical assault and vampirism are a recurrent feature of popular explanations of misfortune in Tuva, South Siberia. Based on a field study of healing practices in an “Association of Shamans”, this article analyses rituals of redressing curse afflictions in the context of Russian political domination. A central purpose of this discussion is to foreground the centrality of kinds of parasitical worship and occult threat to structures of political power in—and beyond—the territory of Tuva. Focusing on a “cursescape”, which develops from the combative practices of shamans, occult specialists, and office-holders, the article probes a repertoire of shamanic healing symbols. It is argued that healing efficacy is constructed in the process of engaging with hunting symbols and animal spirits, which appear in Indigenous Siberian cosmologies. The analysis shows that ideas of ritual risk underpin the process of symbolic resolution. Whereas shamanic practices provide refuge to spirits evicted from their natural landscapes, Tibetan Buddhism—the unifying religion of Tuva—offers an alternative path of healing the effects of the shamans’ propagation of spirits. The article highlights indigenous perceptions of a “cursed” landscape as a space where the agencies of “darkness” and their political sponsors are confronted with an emancipating religious modality emerging from local Buddhist rituals. The analysis displays the unsolved drama of itinerant spirits and shamanic ancestral souls, whose agency is revealed through successive—yet inauspicious—forms of reincarnation. Full article
(This article belongs to the Special Issue Religion, Ritual, and Healing)
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<p>A herders’ camp, consisting of two yurts (the abodes of two ethnic Tuvan families having common descent) and a wooden corral used for enclosing their livestock. This site was located on the slopes of a mountain range approximately two hours away from the township of Ak-Dovurak in the west Tuvan basin (a small town that is synonymous with its local asbestos mining plant).</p>
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<p>A snapshot of the white nightfall during a stroll around the empty (yet really safe) streets of Erzin village. The right side of this long road was interspersed with wooden houses, separated from each other by small fences, like the “house” (<span class="html-italic">bazhyŋ</span>; Tuvan), owned by the shaman who hosted this author one evening in February 2003. The term “bazhyŋ” (pronounced with a nasal -n-) denotes both a “house”, involving a family compound (<span class="html-italic">dom</span>, Russian) and an apartment (<span class="html-italic">kvartira</span>, Russian). The latter is typical of Soviet-era residential units in Kyzyl, as well as in other towns of Tuva (and broadly in Russia). During his fieldwork in Kyzyl, this author lived in a rental apartment in an outlying residential area known as <span class="html-italic">Angarskii Bul’var</span> (nearly a five minute driving distance from the central square of Kyzyl, a town of approximately 115,000 residents).</p>
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<p>The shaman in action: the Headman performing a kamlaniye ritual for a client in the main consultation room of his Association.</p>
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<p>A rare cultic object and a symbol of Northern Shamanism, this “eeren” is the abode of the Headman’s shamanic ancestral spirit. The bulk of loose threads that form the effigy’s body derives from previous rituals of “cutting” lines of cursing, which the Headman practiced for his clients.</p>
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<p>Overseeing the Headman’s rituals from its altar, the consecrated bear presides over an assemblage of “pagan idols”, such as frightening masks, an embalmed raven, and a skull of a predatory animal with its sharp teeth. The Headman’s brown shamanic gown, which is decorated with shreds of fur and numerous paraphernalia (such as a copper mirror and several tiny bells), is hung behind his chair and desk.</p>
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<p>The Headman (first on the right) organizing a ceremonial procession of shamans addressing the “Bear Spirit” with prayers at the Association’s fenced courtyard. The ritual took place a few hours after a communal meal including fresh boiled meat from a sheep slaughtered for this occasion. As was customary, large-scale rituals of ancestral (or spirit) worship were being officiated by the Headman either at his Association’s site or in “sacred places” (<span class="html-italic">sviashchennyie mesta</span>, Russian) in the taiga. Often times, an “audience” of pilgrims, the majority of them being relatives of the shamans, was present at these rituals—including even occasional foreign visitors and neo-shamanic pilgrims as an index of a cosmopolitan landscape, where digital cameras and recorders became indispensable “shamanic tools”. Hence, the boundary between “shamanic performance” as a venue for sensationalism and “ritual” as an act of a real devotional “call” was not always as clear-cut as traditionalists or die-hard cultural conservatives would prefer this to be.</p>
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<p>Author’s reconstruction of divinatory map showing a stream of curses that struck the client and her relative, killing the latter. The diagram lays out in a schematic fashion the pattern of multilateral curse affliction, as it emerged from the Headman’s divination. The invasion of curses is featured by the two curved red arrows, which represent the reflexive or spiraling motion of ballistic supernatural weapons deployed by either murderous sorcerers or specialists in intercepting curses (namely, weapons similar to “surface-to-air” missiles, in the Headman’s words; “земля-вoздух”, in Russian). The red dotted lines, which extend from each of the black circles, show the path of curses cutting across the victims (the latter ones are symbolized by two white circles right above the central axis of the diagram).</p>
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22 pages, 286 KiB  
Article
Ostrowski-Type Inequalities for Functions of Two Variables in Banach Spaces
by Muhammad Amer Latif and Ohud Bulayhan Almutairi
Mathematics 2024, 12(17), 2748; https://doi.org/10.3390/math12172748 - 4 Sep 2024
Cited by 1 | Viewed by 512
Abstract
In this paper, we offer Ostrowski-type inequalities that extend the findings that have been proven for functions of one variable with values in Banach spaces, conducted in a remarkable study by Dragomir, to functions of two variables containing values in the product Banach [...] Read more.
In this paper, we offer Ostrowski-type inequalities that extend the findings that have been proven for functions of one variable with values in Banach spaces, conducted in a remarkable study by Dragomir, to functions of two variables containing values in the product Banach spaces. Our findings are also an extension of several previous findings that have been established for functions of two variable functions. Prior studies on Ostrowski-type inequalities incriminated functions that have values in Banach spaces or Hilbert spaces. This study is unique and significant in the field of mathematical inequalities, and specifically in the study of Ostrowski-type inequalities, because they have been established for functions having values in a product of two Banach spaces. Full article
(This article belongs to the Special Issue Mathematical Analysis and Functional Analysis and Their Applications)
23 pages, 344 KiB  
Article
On the Equivalence between Differential and Integral Forms of Caputo-Type Fractional Problems on Hölder Spaces
by Mieczysław Cichoń, Hussein A. H. Salem and Wafa Shammakh
Mathematics 2024, 12(17), 2631; https://doi.org/10.3390/math12172631 - 24 Aug 2024
Cited by 3 | Viewed by 910
Abstract
As claimed in many papers, the equivalence between the Caputo-type fractional differential problem and the corresponding integral forms may fail outside the spaces of absolutely continuous functions, even in Hölder spaces. To avoid such an equivalence problem, we define a “new” appropriate fractional [...] Read more.
As claimed in many papers, the equivalence between the Caputo-type fractional differential problem and the corresponding integral forms may fail outside the spaces of absolutely continuous functions, even in Hölder spaces. To avoid such an equivalence problem, we define a “new” appropriate fractional integral operator, which is the right inverse of the Caputo derivative on some Hölder spaces of critical orders less than 1. A series of illustrative examples and counter-examples substantiate the necessity of our research. As an application, we use our method to discuss the BVP for the Langevin fractional differential equation dψβ,μdtβdψα,μdtα+λx(t)=f(t,x(t)),t[a,b],λR, for fC[a,b]×R and some critical orders β,α(0,1), combined with appropriate initial or boundary conditions, and with general classes of ψ-tempered Hilfer problems with ψ-tempered fractional derivatives. The BVP for fractional differential problems of the Bagley–Torvik type was also studied. Full article
15 pages, 20333 KiB  
Article
Elastoplastic and Electrochemical Characterization of xTiB2 Strengthened Ti Porous Composites for Their Potential Biomedical Applications
by David Israel Bravo-Bárcenas, Reynier Suárez-Martínez, Jonatan Pérez-Alvarez, Omar Jiménez-Alemán, Iván Gerardo Farias-Velazquez, Marco Aurelio Gonzaléz-Albarrán and Jorge Chávez
Coatings 2024, 14(8), 991; https://doi.org/10.3390/coatings14080991 - 6 Aug 2024
Viewed by 920
Abstract
The microstructure, elastoplastic properties, and corrosive response of induced porous Ti-TiH2 materials reinforced with TiB2 particles were investigated. Samples were fabricated using CP-Ti Grade1, Titanium Hydride (TiH2), TiB2 powders (0, 3, 10, and 30 vol.%), and ammonium bicarbonate [...] Read more.
The microstructure, elastoplastic properties, and corrosive response of induced porous Ti-TiH2 materials reinforced with TiB2 particles were investigated. Samples were fabricated using CP-Ti Grade1, Titanium Hydride (TiH2), TiB2 powders (0, 3, 10, and 30 vol.%), and ammonium bicarbonate salt (40 vol.%) as a space holder. Composites were fabricated using the Powder Metallurgy technique under high-vacuum conditions (HVS) at 1100 °C. Scanning electron microscopy, X-ray diffraction, nanoindentation tests, and electrochemical assays were used to investigate the pore formation, pore distribution, phase formation, elastoplastic properties, and electrochemical behavior of the compounds, respectively. With a mean pore diameter of 50–900 µm and Young’s modulus of less than 100 GPa, which is close to the properties of human bone, the pore structures of the compounds processed here are shown to be a potential biomaterial for osseointegration. In addition, their H/Er and H3/Er2 ratios for the reinforced samples are higher than those of the unreinforced sample (1.5 and 4 times higher than the unreinforced sample, respectively), suggesting a better wear resistance of the Ti-TiH2/xTiB2 composites. Electrochemical experiments demonstrated that the Ti-TiH2/xTiB2 composites exhibited superior passivation properties compared to the Ti-TiH2 sample. Additionally, the corrosion rates exhibited by the 3 and 10 vol.% of TiB2 samples were found to be within an acceptable range for potential biomedical applications (29.26 and 185.82 E-3 mm·y−1). The elastoplastic properties combined with the electrochemical behavior place the Ti-TiH2/3-10TiB2 composites as potential candidates for the biomedical application of CP-Ti. Full article
(This article belongs to the Special Issue Advanced Alloy Degradation and Implants, 2nd Edition)
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Figure 1
<p>SEM micrographs of the Ti-TiH<sub>2</sub>: (<b>a</b>) U, (<b>b</b>) R3, (<b>c</b>) R10, and (<b>d</b>) R30 compounds.</p>
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<p>Pore diameter variation of the compounds: (<b>a</b>) U, (<b>b</b>) R3, (<b>c</b>) R10 and, (<b>d</b>) R30 sample.</p>
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<p>Behavior of the relative density of the compounds.</p>
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<p>XRD resultant pattern of the composites.</p>
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<p>SEM images and EDS spectrums for the (<b>a</b>) U, (<b>b</b>) R3, (<b>c</b>) R10, and (<b>d</b>) R30 samples.</p>
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<p>SEM images and EDS spectrums for the (<b>a</b>) U, (<b>b</b>) R3, (<b>c</b>) R10, and (<b>d</b>) R30 samples.</p>
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<p>(<b>a</b>) Nanohardness (<span class="html-italic">H</span>) vs. reduced elastic modulus (<span class="html-italic">E<sub>r</sub></span>), and (<b>b</b>) the <span class="html-italic">H</span>/<span class="html-italic">E<sub>r</sub></span> and <span class="html-italic">H</span><sup>3</sup>/<span class="html-italic">E<sub>r</sub></span><sup>2</sup> ratios of the U and R samples.</p>
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<p>(<b>a</b>) The OCP and, (<b>b</b>) Tafel plots behavior of the composites.</p>
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<p>Electrochemical behavior of composites: (<b>a</b>) EIS Nyquist plots. (<b>b</b>) and (<b>c</b>) EIS Bode plots. (<b>d</b>) EIS equivalent circuit for the U sample and, (<b>e</b>) EIS equivalent circuit for the R samples.</p>
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<p>BSE micrographs and semiquantitative analysis of the (<b>a</b>) U, (<b>b</b>) R3, (<b>c</b>) R10, and (<b>d</b>) R30 compounds.</p>
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13 pages, 6805 KiB  
Article
High–Strength Porous TiNbZrTaFe Alloys Fabricated by Sintering of Nanocomposite Powder Precursor with Space Holder Technique
by Yuhua Li, Yuxin He, Rong Zhao, Libin Niu, Juxin Qu and Lai-Chang Zhang
Metals 2024, 14(7), 824; https://doi.org/10.3390/met14070824 - 18 Jul 2024
Cited by 1 | Viewed by 1299
Abstract
Although introducing high porosity in biomedical Ti alloys can reduce their elastic modulus and promote new bone ingrowth, relieving the stress–shielding effect and implant failure, this also causes a decline in the alloys’ mechanical strength. In this work, a new preparation method for [...] Read more.
Although introducing high porosity in biomedical Ti alloys can reduce their elastic modulus and promote new bone ingrowth, relieving the stress–shielding effect and implant failure, this also causes a decline in the alloys’ mechanical strength. In this work, a new preparation method for the high–strength and high–porosity Ti65Nb23.33Zr5Ta1.67Fe5 (TNZTF, at.%) alloy was suggested by sintering nanocomposite powder precursor in combination with the use of a space holder technique, in which NH4HCO3 is adopted to achieve a porous structure. The highly porous TNZTF alloy possesses a homogeneous fine–grained microstructure consisting of equiaxed α–Ti and a small amount of FeTi2, the latter of which is distributed in the β–Ti matrix. Through adjusting the mass fraction of NH4HCO3, a novel high–porosity, and high–strength TNZTF alloy with a low modulus was successfully prepared. The porous alloy with the addition of 30 wt.% NH4HCO3 exhibits a porosity of 50.3 ± 0.2%, a maximum strength of 327.3 ± 2.1 MPa, and an elastic modulus of 12.2 ± 0.3 GPa. The strength enhancement is mainly attributed to the unique fine–grained microstructure, which is obtained by the crystallization of the amorphous phase and the ductile–brittle mixed fracture mechanism. The prepared porous TNZTF alloy possesses higher mechanical strength and well–matched elastic modulus, showing great potential as an implant material. Full article
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<p>(<b>a</b>) XRD pattern, (<b>b</b>) DSC curve, (<b>c</b>) SEM morphology, and (<b>d</b>) TEM bright–field image and corresponding selected area diffraction (SAED) pattern of the 115 h–milled TNZTF powder.</p>
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<p>Effect of NH<sub>4</sub>HCO<sub>3</sub> addition on the porosity of the as–fabricated porous TNZTF samples.</p>
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<p>Pore morphologies of the as–fabricated porous TNZTF samples and the corresponding pore images after binarization: (<b>a</b>,<b>b</b>) S30, (<b>c</b>,<b>d</b>) S40, and (<b>e</b>,<b>f</b>) S50.</p>
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<p>Pore size distribution of the as–fabricated porous TNZTF samples: (<b>a</b>) S30, (<b>b</b>) S40, and (<b>c</b>) S50; (<b>d</b>) relationship between roundness and pore diameter for S30.</p>
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<p>Pore roundness distribution of the as–fabricated porous TNZTF samples: (<b>a</b>) S30, (<b>b</b>) S40, and (<b>c</b>) S50; (<b>d</b>) relationship between roundness and pore diameter for S50.</p>
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<p>XRD patterns and SEM microstructures of the as–fabricated porous TNZTF samples.</p>
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<p>Compressive stress–strain curves of the as–fabricated porous TNZTF samples.</p>
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<p>SEM fracture morphologies at low and high magnification of the as–fabricated porous TNZTF samples: (<b>a</b>,<b>b</b>) S30, (<b>c</b>,<b>d</b>) S40, and (<b>e</b>,<b>f</b>) S50.</p>
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21 pages, 19521 KiB  
Article
Ultrathin Carbon Textures Produced on Machined Surfaces in an Integrated Finishing Process Using Microabrasive Films
by Katarzyna Tandecka, Wojciech Kacalak, Michał Wieczorowski, Krzysztof Rokosz, Patrick Chapon and Thomas G. Mathia
Materials 2024, 17(14), 3456; https://doi.org/10.3390/ma17143456 - 12 Jul 2024
Cited by 3 | Viewed by 793
Abstract
This study presents research into the unique method of depositing carbon layers onto processed surfaces, during finishing with abrasive films, on a global basis. The authors of this article are holders of the patent for this method. What makes this technology outstanding is [...] Read more.
This study presents research into the unique method of depositing carbon layers onto processed surfaces, during finishing with abrasive films, on a global basis. The authors of this article are holders of the patent for this method. What makes this technology outstanding is that it integrates processes, whereby micro-finishing and the deposition of a carbon layer onto freshly exposed surface fragments is achieved simultaneously, in a single process. Among the main advantages accruable from this process is the reduction of surface irregularities, while the deposition of a carbon layer is achieved simultaneously. Ultrathin graphite layers can be widely used in conditions where other methods of reducing the coefficient of friction are not possible, such as in regard to micromechanisms. This article illustrates the application of carbon coating, end on, on a surface processed with abrasive film, containing intergranular spaces, saturated with graphite. Thin carbon layers were obtained on two substrates that did not contain carbon in their initial composition: soda–lime glass and a tin–bronze alloy. It was performed through microscopic examinations of the produced surface, roughness analyses of these surfaces, and analysis of the chemical compositions determined by two methods, namely EDS and GDOES, proving the existence of the coatings. The aim of this paper is to prove the possibility and efficiency of using graphite-impregnated lapping films in the deposition process of carbon films, with improved surface smoothness, durability, and wear resistance. The produced coatings will be tested in regard to their operational properties in further research. The authors underline the potential of this method to revolutionize surface treatment processes, due to the significant advantages it offers across various industries. Full article
(This article belongs to the Special Issue Advances in Metal Coatings for Wear and Corrosion Applications)
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<p>Kinematic diagram of rotary surface superfinishing using lapping films, indicating the following quantities: <span class="html-italic">v<sub>t</sub></span>—tool velocity, <span class="html-italic">v<sub>w</sub></span>—workpiece velocity, <span class="html-italic">v<sub>f</sub></span>—tool feed rate, <span class="html-italic">f<sub>o</sub></span>—tool oscillation rate, and <span class="html-italic">F<sub>r</sub></span>—the pressure force of the pressing roller [<a href="#B43-materials-17-03456" class="html-bibr">43</a>].</p>
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<p>Kinematic diagram of finishing with the simultaneous application of a thin graphite coating on the finished surface, indicating the following quantities: <span class="html-italic">v<sub>t</sub></span>—tool velocity, <span class="html-italic">v<sub>w</sub></span>—workpiece velocity, <span class="html-italic">f<sub>o</sub></span>—tool oscillation rate, and <span class="html-italic">F<sub>r</sub></span>—the pressure force of the pressing roller.</p>
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<p>Research setup for the micro-finishing process, with the integrated simultaneous application of thin carbon layers.</p>
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<p>Workpiece before the lapping film process and after the smoothing process, with marked measurement inserts as detachable elements.</p>
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<p>Comparison of soda–lime glass surface finishes: Left: Surface finished with conventional lapping film. Right: Surface finished with lapping film, where intergranular spaces are saturated with graphite. Below: Elemental composition and weight percentages for each surface.</p>
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<p>SEM images of the soda–lime glass surface after the micro-finishing process, with a thin carbon layer applied in the form of visible bands.</p>
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<p>Soda–lime glass topography. (<b>a</b>) Conventional soda–lime glass surface. (<b>b</b>) Surface finished with abrasive films and carbon layer. Insets: Magnified view of the highlighted area in each topography map.</p>
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<p>Graphite texture formed on the machined surface. Areas with the highest probability of carbon accumulation in the valleys of machining marks.</p>
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<p>Confocal microscope images in optical mode of the soda–lime glass surface sample after lapping. (<b>a</b>) Conventional soda–lime glass surface. (<b>b</b>) Surface finished with abrasive films and a carbon layer.</p>
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<p>Surface roughness parameters between the conventional surface and the surface with a carbon layer, in micrometers. The parameters measured are the maximum surface height (Sz), maximum valley depth (Sv), and maximum peak height (Sp) in µm.</p>
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<p>Plot of carbon signal (C 156 nm) versus diode spraying time for surfaces with and without a carbon layer.</p>
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<p>Plot of oxygen signal (O 130 nm) versus diode spraying time for surfaces with and without a carbon layer.</p>
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<p>Chemical composition analysis of the surface of the CuSn7Zn4Pb6/RG7 tin–bronze alloy after carbon coating. Top left is the SEM micrograph of the surface, the images on the right are the elemental distribution maps for carbon (C), copper (Cu), and tin (Sn). The bottom chart shows the atomic percentage composition of the detected elements and the measurement certainty: Cu 90.7% (0.99), C 6.6% (0.94), Sn 2.8% (0.94).</p>
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<p>Conventionally finished tin–bronze surface.</p>
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<p>Tin–bronze surface finished with abrasive film and a carbon layer.</p>
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<p>Surface roughness parameters of the bronze sample with a conventional surface and a carbon layer. The parameters measured are the maximum surface height (Sz), maximum valley depth (Sv), and maximum peak height (Sp) in µm.</p>
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<p>Confocal microscope images in optical mode, showing the true colors of the bronze alloy surface sample after the lapping process: (<b>a</b>) conventional finish and (<b>b</b>) finish with abrasive films and a carbon layer.</p>
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