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19 pages, 3225 KiB  
Article
Tailoring Thermomechanical, Shape Memory and Self-Healing Properties of Furan-Based Polyketone via Diels-Alder Chemistry with Different Bismaleimide Crosslinkers
by Esteban Araya-Hermosilla, Marco Carlotti, Felipe Orozco, Guilherme Macedo R. Lima, Rodrigo Araya-Hermosilla, Daniela E. Ortega, Diego Cortés-Arriagada, Francesco Picchioni, Ranjita K. Bose, Virgilio Mattoli and Andrea Pucci
Polymers 2025, 17(5), 565; https://doi.org/10.3390/polym17050565 (registering DOI) - 20 Feb 2025
Abstract
Furan/maleimide dynamic covalent chemistry has been extensively used to fabricate re-workable and self-healing thermosets. Understanding the relationship between crosslinker structure, network dynamics, and material final properties, however, remains a challenge. This study introduces self-healing and shape-memory thermosets derived from furan-functionalized polyketones (PKFU) crosslinked [...] Read more.
Furan/maleimide dynamic covalent chemistry has been extensively used to fabricate re-workable and self-healing thermosets. Understanding the relationship between crosslinker structure, network dynamics, and material final properties, however, remains a challenge. This study introduces self-healing and shape-memory thermosets derived from furan-functionalized polyketones (PKFU) crosslinked with aromatic bis-maleimides, i.e., 1,1′-(methylenedi-4,1-phenylene)bis-maleimide (BISM1) and bis(3-ethyl-5-methyl-4-maleimidophenyl)methane (BISM2), via a thermally reversible Diels-Alder reaction. Polyketones were chemically modified with furfurylamine through the Paal-Knorr reaction, achieving varying furan grafting ratios. The resulting networks, characterized by ATR-FTIR, 1H-NMR, gel permeation chromatography (GPC), differential scanning calorimetry (DSC), and rheology, demonstrated tunable thermomechanical properties. BISM2-based thermosets exhibited enhanced thermal stability and reversibility over a broad temperature range (20–120 °C), with a shape recovery ratio of up to 89% and complete self-healing at 120 °C within 5 min. These findings highlight the potential of polyketone-based thermosets for applications requiring adaptive thermomechanical properties, efficient self-repair, and sustainability. Full article
(This article belongs to the Section Polymer Chemistry)
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Figure 1
<p>(<b>a</b>) Schematic representation of PK0 chemically modified with furfurylamine via the Paal–Knorr reaction (PK0FU), bismaleimides BISM1 and BISM2 used in the crosslinking process, and the resulting thermoreversible thermoset. (<b>b</b>) ATR–FTIR and (<b>c</b>) <sup>1</sup>H–NMR spectra of PK0 and modified with FU at different CO % (PKFU20, PKFU40, PKFU60, PKFU80). (<b>d</b>) PKFUs T<sub>g</sub> at different di-carbonyl conversion (CO %) calculated from DSC analysis (see <a href="#app1-polymers-17-00565" class="html-app">Figure S2</a> for full thermal history and all polymer series).</p>
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<p>(<b>a</b>) temperature and (<b>b</b>) energy required for rDA reaction in polyketone thermosets crosslinked with BISM1 and (<b>c</b>) temperature and (<b>d</b>) energy required for rDA reaction in polyketone thermosets crosslinked with BISM2, plotted as a function of carbonyl conversion.</p>
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<p>(<b>a</b>) Enthalpy reaction pathways of endo-(black) and exo−(red) stereoisomers for the Diels-Alder cycloaddition reactions with BISM1 as a dienophile. (<b>b</b>) Enthalpy reaction pathways of endo-(black) and exo−(red) stereoisomers for the Diels−Alder cycloaddition reactions with BISM2 as a dienophile. (<b>c</b>) Distortion-interaction analysis in the P1 endo and exo product structures according to <a href="#polymers-17-00565-f003" class="html-fig">Figure 3</a>a,b. Fragment 1 is the BISM1 or BISM2 dienophiles, and fragment 2 is the furan−PK diene. ΔE<sub>dist−BISM1</sub> and ΔE<sub>dist−BISM2</sub> represent the distortion energy of BISM1 and BISM2 dienophiles, respectively, while ΔE<sub>dist−furanPK</sub> represents the distortion energy of diene. ΔE<sub>int represents</sub> the interaction energy between each dienophile and diene molecule.</p>
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<p>Softening point trend of the polyketone thermosets at different conversion percentages.</p>
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<p>(<b>a</b>) Thermomechanical properties (complex modulus G*) and (<b>b</b>) Softening point (Tan δ) of the PK0FU40 and PK0FU60 crosslinked at a molar ratio of 1:0.5 FU:BISM with BISM1 and BISM2 determined by rheology.</p>
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<p>Thermomechanical properties (complex modulus G*) PK0FU40 crosslinked with BISM2 at different molar ratios 1:0.67, 1:0.5, and 1:0.33 FU: BISM determined by rheology.</p>
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<p>(<b>a</b>) Energy required for rDA reaction, (<b>b</b>) maximum temperature energy required for rDA reaction, onset of the temperature required for rDA, and T<sub>g</sub> for thermosets composed by PK0FU40 crosslinked with BISM2 at different molar ratios 1:0.67, 1:0.5, and 1:0.33 FU:BISM determined by DSC.</p>
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<p>Self-healing test of thermoset PK0FU40 and BISM2 at a 1:0.5 (FU:BISM) at a 1:0.5 (FU:BISM) crosslinking molar ratio after (<b>a</b>) scratching and (<b>b</b>) thermal treatment at 120 °C for 5 min.</p>
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1 pages, 128 KiB  
Correction
Correction: Staszczak et al. Nucleation, Development and Healing of Micro-Cracks in Shape Memory Polyurethane Subjected to Subsequent Tension Cycles. Polymers 2024, 16, 1930
by Maria Staszczak, Leszek Urbański, Arkadiusz Gradys, Mariana Cristea and Elżbieta Alicja Pieczyska
Polymers 2025, 17(5), 560; https://doi.org/10.3390/polym17050560 - 20 Feb 2025
Abstract
In the original publication [...] Full article
22 pages, 6734 KiB  
Article
Envelope Morphology of an Elephant Trunk-like Robot Based on Differential Cable–SMA Spring Actuation
by Longfei Sun and Huiying Gu
Actuators 2025, 14(2), 100; https://doi.org/10.3390/act14020100 - 19 Feb 2025
Abstract
Most trunk-like robots are designed with distributed actuators to mimic the envelope-grasping behavior of elephant trunks in nature, leading to a complex actuation system. In this paper, a modular underactuated elephant trunk-imitating robot based on the combined drive of the cable and shape [...] Read more.
Most trunk-like robots are designed with distributed actuators to mimic the envelope-grasping behavior of elephant trunks in nature, leading to a complex actuation system. In this paper, a modular underactuated elephant trunk-imitating robot based on the combined drive of the cable and shape memory alloy (SMA) springs is designed. Unlike the traditional underactuated structure that can only passively adapt to the envelope of the object contour, the proposed elephant trunk robot can control the cable tension and the equivalent stiffness of the SMA springs to achieve active control of the envelope morphology for different target objects. The overall structure of the elephant trunk robot is designed and the principle of deformation envelope is elucidated. Based on the static model of the robot under load, the mapping relationship between the tension force and the tension angle between modules is derived. The positive kinematic model of the elephant trunk robot is established based on the Debavit–Hartenberg (D–H) method, the spatial position of the elephant trunk robot is obtained, and the Monte Carlo method is used to derive the robot’s working space. The active bending envelope grasping performance is further verified by building the prototype to perform grasping experiments on objects of various shapes. Full article
(This article belongs to the Section Actuators for Robotics)
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Figure 1
<p>Elephant trunk function: (<b>a</b>) Elephant trunk muscle composition; (<b>b</b>) Elephant trunk curled objects.</p>
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<p>Elephant trunk structure: (<b>a</b>) Elephant trunk [<a href="#B19-actuators-14-00100" class="html-bibr">19</a>]; (<b>b</b>) 3D model of elephant trunk-like robot; (<b>c</b>) Modular structure.</p>
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<p>3D model of the unit module: (<b>a</b>) Front view; (<b>b</b>) Back view.</p>
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<p>Force analysis: (<b>a</b>) Simplified model; (<b>b</b>) Mechanical model.</p>
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<p>Robot envelope morphology: (<b>a</b>) Envelope spherical body; (<b>b</b>) Envelope trapezoid; (<b>c</b>) Envelope polygon.</p>
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<p>D–H Coordinate system of elephant trunk robot.</p>
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<p>Workspace: (<b>a</b>) Three-dimensional view of the workspace; (<b>b</b>) Workspace projection in x–y plane.</p>
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<p>Adams model of elephant trunk robot: (<b>a</b>) Adams model (<b>b</b>) Tension spring damper setting (<b>c</b>) Back view.</p>
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<p>Angle curve for elephant trunk robot: (<b>a</b>) Group 1; (<b>b</b>) Group 2; (<b>c</b>) Group 3; (<b>d</b>) Group 4.</p>
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<p>Simulation results of robot envelope morphology: (<b>a</b>) Group 1 (<span class="html-italic">F</span> = 18.8 N, <span class="html-italic">R</span><sub>1</sub> ≈ 18 mm); (<b>b</b>) Group 2 (<span class="html-italic">F</span> = 11.7 N, <span class="html-italic">R</span><sub>2</sub> ≈ 28 mm) (<b>c</b>) Group 3 (<span class="html-italic">F</span> = 7.8 N, <span class="html-italic">R</span><sub>3</sub> ≈ 50 mm); (<b>d</b>) Group 4 (<span class="html-italic">F</span> = 11.3 N, <span class="html-italic">R</span><sub>4</sub> ≈ 80 mm).</p>
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<p>Elephant trunk robot prototype.</p>
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<p>Experimental system components.</p>
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<p>The control system of the elephant trunk robot.</p>
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<p>Mechanical property test experiment of SMA spring.</p>
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<p>SMA spring tension response.</p>
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<p>Variation of contraction force and elongation of SMA spring.</p>
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<p>Elephant trunk envelope morphology: (<b>a</b>) <span class="html-italic">F</span><sub>1</sub> = 8 N; (<b>b</b>) <span class="html-italic">F</span><sub>2</sub> = 10 N; (<b>c</b>) <span class="html-italic">F</span><sub>3</sub> = 12 N.</p>
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<p>Elephant trunk robot grasps objects: (<b>a</b>) Envelope egg (without active SMA springs); (<b>b</b>) Envelope tennis; (<b>c</b>) Envelope cube; (<b>d</b>) Envelope cup; (<b>e</b>) Envelope apple; (<b>f</b>) Envelope cylinder.</p>
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20 pages, 17189 KiB  
Article
Parametric Study on Investigations of GMAW-Based WAAM Process Parameters and Effect on Microstructure and Mechanical Properties of NiTi SMA
by Vatsal Vaghasia, Rakesh Chaudhari, Vivek K. Patel and Jay Vora
J. Manuf. Mater. Process. 2025, 9(2), 58; https://doi.org/10.3390/jmmp9020058 - 13 Feb 2025
Abstract
In the present study, an attempt was made to build a thin-walled structure consisting of 10 layers using nitinol wire on a titanium substrate via a gas–metal arc welding (GMAW)-based wire-arc additive manufacturing (WAAM) process. A thin-walled structure was fabricated by using nitinol [...] Read more.
In the present study, an attempt was made to build a thin-walled structure consisting of 10 layers using nitinol wire on a titanium substrate via a gas–metal arc welding (GMAW)-based wire-arc additive manufacturing (WAAM) process. A thin-walled structure was fabricated by using nitinol wire on a titanium substrate at the optimized parameters of a wire feed speed of 6 m/min, a travel speed of 12 mm/s, and a voltage of 20 V. In a microstructural study, the heat-affected zone was observed to have coarse grains and be columnar in shape, and the first layer exhibited a mix of dendritic structures. The mid-layers demonstrated a mix of coarse and fine columnar grains with dendritic colonies, while the last few layers demonstrated fairly equiaxed grains as well as a finer microstructure, as the cooling rates were very slow. The ultimate tensile strengths (UTSs) obtained at the bottom and top portions were found to be 536.22 MPa and 586.31 MPa. Elongation (EL) degrees of 10.72% and 11.57% were observed in the bottom and top portions, respectively. The fractography of the tensile specimen showed good toughness and ductility of the fabricated nitinol specimen. A microhardness examination showed a minimum value of 236.56 HV in the bottom layer and a maximum value of 316.78 HV in the topmost layer. Full article
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<p>The GMAW-based WAAM experimental setup.</p>
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<p>Determination of bead morphologies, BW and BH.</p>
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<p>Process chart of the HTS algorithm [<a href="#B44-jmmp-09-00058" class="html-bibr">44</a>].</p>
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<p>A 10-layered nitinol specimen fabricated by WAAM at optimized parameters.</p>
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<p>Testing locations of the built structure.</p>
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<p>Single-layer depositions along with cut cross-sections of depositions.</p>
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<p>Influences of WAAM variables on BH response.</p>
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<p>Influences of WAAM variables on BW response.</p>
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<p>Macrostructure of the built WAAM structure.</p>
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<p>Microstructures of (<b>a</b>) HAZ and initial layers, (<b>b</b>) middle layers, and (<b>c</b>) top layers of the built WAAM structure.</p>
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<p>Microstructures of (<b>a</b>) HAZ and initial layers, (<b>b</b>) middle layers, and (<b>c</b>) top layers of the built WAAM structure.</p>
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<p>Tensile test specimens (<b>a</b>) after fracture and (<b>b</b>) after fractography.</p>
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<p>Microhardness along the build direction for a WAAM structure of nitinol SMA.</p>
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17 pages, 7657 KiB  
Article
Microstructure, Thermal, and Mechanical Behavior of NiTi Shape Memory Alloy Obtained by Micro Wire and Arc Direct Energy Deposition
by Tadeu C. da Silva, Edwin Sallica-Leva, Emilio Rayón, Claudio T. Santos, João C. A. D. Filho, Neri Volpato, Dalton D. Lima, Paulo H. G. Dornelas, Sergio S. M. Tavares and Telmo G. Santos
J. Manuf. Mater. Process. 2025, 9(2), 57; https://doi.org/10.3390/jmmp9020057 - 13 Feb 2025
Abstract
Additive manufacturing (AM) is revolutionizing the fabrication of metallic components, offering significant potential to compete with or complement traditional casting, forging, and machining processes, and enabling the production of complex functional components. Recent advancements in AM technology have facilitated the processing of shape [...] Read more.
Additive manufacturing (AM) is revolutionizing the fabrication of metallic components, offering significant potential to compete with or complement traditional casting, forging, and machining processes, and enabling the production of complex functional components. Recent advancements in AM technology have facilitated the processing of shape memory alloys (SMAs) with functional properties comparable to those of conventionally processed alloys. However, the AM of NiTi SMAs remains underexplored due to the extreme complexity of the process, high melting point, and reactivity with oxygen. This study investigates the impact of AM processing on the shape memory properties of NiTi alloys using the Micro Wire and Arc Directed Energy Deposition (μ-WA-DED) technique in short circuit mode with a pioneering 0.3 mm pre-alloyed wire, focusing on increasing precision and control in the deposition process. The macroscopic morphology, microstructure, phase composition, phase-transformation temperatures, and mechanical properties of each deposited layer were analyzed. Results indicated austenite (B2) as the predominant phase, with retained martensite (B19′) and a reversible martensitic transformation (B2 ⇌ B19′) in the second layer. Mechanical characterization revealed variations in hardness (H) and elastic modulus (E) due to microstructural heterogeneity and composition. The first layer exhibited H = 3.8 GPa and E = 70 GPa, associated with the B2-NiTi phase, while higher values were obtained in the second layer, i.e., E = 100 GPa and H = 7 GPa. This study establishes for the first time the feasibility of NiTi alloy deposition with a 0.3 mm wire, setting a new standard for future research and applications in AM using μ-WA-DED. Full article
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<p>Schematic representation of the employed deposition strategy that was used to manufacture the NiTi walls by µ-WA-DED.</p>
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<p>(<b>a</b>) Schematic representation of the layer deposition with emphasis on the region analyzed by SEM, (<b>b</b>) cross-section along the longitudinal direction after metallographic preparation of the sample, (<b>c</b>) panoramic image of the printed NiTi part, and (<b>d</b>) 0.3 mm NiTi wire acquired from Fort Wayne Metals (Fort Wayne, IN, USA). BD: build direction.</p>
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<p>FESEM-BSE images of the microstructure in the (<b>a</b>,<b>b</b>) 1st and (<b>c</b>,<b>d</b>) 2nd layer with (<b>a</b>,<b>c</b>) low and (<b>b</b>,<b>d</b>) high magnification, highlighting the EDS analysis locations in the higher magnification images (i.e., (<b>b</b>,<b>d</b>)).</p>
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<p>FESEM-BSE high magnification image of the microstructure in the 2nd layer of the NiTi part.</p>
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<p>XRD patterns of the 1st and 2nd layers of the NiTi part.</p>
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<p>DSC curves of the NiTi part: (<b>a</b>) 1st layer; (<b>b</b>) 2nd layer and 2nd layer (cycled).</p>
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<p>(<b>a</b>) OM image of the cross-section of the printed NiTi part. (<b>b</b>) OM magnified image of the red-rectangle region highlighted in (<b>a</b>), showing the location of nanoindentation imprints. (<b>c</b>–<b>e</b>) FESEM-BSE images of the imprints localized in the two-dimensional array (<b>c</b>) and in the linear array (<b>d</b>,<b>e</b>).</p>
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<p>Extracted E and H values of the NiTi part as a function of the distance from the top side of the 2nd layer, denoted by a, to the bottom side of the 1st layer, denoted by f.</p>
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<p>E (<b>a</b>,<b>c</b>) and H (<b>b</b>,<b>d</b>) histograms of the NiTi part for the 1st (<b>a</b>,<b>b</b>) and 2nd (<b>c</b>,<b>d</b>) layer.</p>
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33 pages, 13703 KiB  
Article
A Holistic and Critical Exploration of Cultural Significance of a Reconstructed Heritage Site: Bursa Mevlevi Lodge
by Duygu Gök, Gizem Durmuş, Bengisu Özkılavuz, Elif Acar and Saadet Gündoğdu
Buildings 2025, 15(4), 568; https://doi.org/10.3390/buildings15040568 - 12 Feb 2025
Abstract
The city of Bursa has a multi-cultural background and hosts a diverse architectural heritage inherited from the Roman, Byzantine, Ottoman, and Republican periods. A lost architectural and urban heritage of the city is the Bursa Mevlevi Lodge, which was built between the 17th [...] Read more.
The city of Bursa has a multi-cultural background and hosts a diverse architectural heritage inherited from the Roman, Byzantine, Ottoman, and Republican periods. A lost architectural and urban heritage of the city is the Bursa Mevlevi Lodge, which was built between the 17th and 19th centuries. After all the dervish lodges were closed by a law enacted in 1925, Bursa Mevlevi Lodge lost its original function, too. The complex was used for public, residential, and religious purposes until it was demolished in the 1950s due to neglect and abandonment and lost its place in urban memory. Recently, the complex was reconstructed in 2023 and re-functioned as a museum related to Mevlevi culture and Semahane. This article aims to analyze the history and architecture of the complex in the context of Mevlevi culture and Ottoman Mevlevi Lodge architecture. In conclusion, the article reveals that the authenticity of the complex is that it is shaped around the Semahane and identifies its tangible and intangible values and cultural significance in terms of urban history. The article also discusses the justification of the reconstruction as “a controversial heritage conservation method” and the concept of authenticity in the context of contemporary architectural conservation theory. Full article
(This article belongs to the Section Building Materials, and Repair & Renovation)
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<p>The stages of Mevlevi ritual performed in Semahane [<a href="#B8-buildings-15-00568" class="html-bibr">8</a>].</p>
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<p>Semahane (whirl ritual area) picture, the symbolic meaning of the Sema ritual that schematizes the cycle of the soul’s maturation process [<a href="#B31-buildings-15-00568" class="html-bibr">31</a>].</p>
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<p>The 1862 Bursa city map by Suphi Bey showing the location of Bursa Mevlevi Lodge (in yellow circle) in its urban context [<a href="#B41-buildings-15-00568" class="html-bibr">41</a>].</p>
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<p>The timeline showing the history of the Bursa Mevlevi Lodge (created by authors).</p>
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<p>In 2000, the water tank in the Mevlevihane area (<b>left</b>) and the tomb of the Bursa Mevlevi Lodge (<b>right</b>), which was rebuilt in 1953 [<a href="#B41-buildings-15-00568" class="html-bibr">41</a>].</p>
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<p>Foundation research excavation made in 2018 (<b>left</b>) and image of a 3D point cloud of the survey (<b>right</b>) [<a href="#B43-buildings-15-00568" class="html-bibr">43</a>].</p>
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<p>Images taken during the reconstruction of the Bursa Mevlevi Lodge and showing the structural system and materials (Sources: (<b>a</b>) [<a href="#B43-buildings-15-00568" class="html-bibr">43</a>]; (<b>b</b>) [<a href="#B46-buildings-15-00568" class="html-bibr">46</a>]; (<b>c</b>) [<a href="#B47-buildings-15-00568" class="html-bibr">47</a>]; (<b>d</b>) [<a href="#B48-buildings-15-00568" class="html-bibr">48</a>]).</p>
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<p>The site plan of Bursa Mevlevi Lodge complex after reconstruction (The site plan sketch was prepared by modifying the drawing taken from the Bursa Metropolitan Municipality Archive [<a href="#B41-buildings-15-00568" class="html-bibr">41</a>]).</p>
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<p>The new entrance through the parking lot (<b>left</b>) and the original gate of the complex on Bayramyeri Street (<b>right</b>) (photo taken by author).</p>
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<p>Bursa Mevlevi Lodge site plan restitution drawing (the master plan has been reproduced from [<a href="#B43-buildings-15-00568" class="html-bibr">43</a>], created by authors).</p>
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<p>Semicircular mihrab niche and the balcony above it [<a href="#B41-buildings-15-00568" class="html-bibr">41</a>] and the current condition of the facade (photo taken by author).</p>
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<p>North facade of the Semahane in 1953 (<b>left</b>) [<a href="#B41-buildings-15-00568" class="html-bibr">41</a>] and floral ornaments on the walls of the north facade of the building after reconstruction (<b>right</b>) (photo taken by author).</p>
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<p>The wooden structure of the dome inside the Semahane (Old photos: [<a href="#B41-buildings-15-00568" class="html-bibr">41</a>]; New photos: (photo taken by author).</p>
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<p>The square patterned ceiling of the Semahane in 1953 and its condition after reconstruction (Old photo (<b>left</b>): [<a href="#B41-buildings-15-00568" class="html-bibr">41</a>]; New photo (<b>right</b>): (photo taken by author).</p>
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<p>Sema ritual in the Bursa Mevlevi Lodge (photo taken by author).</p>
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<p>Matbah-ı Şerif, Meydan-ı Şerif, and Tomb (Old photo: [<a href="#B41-buildings-15-00568" class="html-bibr">41</a>]; New photo: (photo taken by author).</p>
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<p>The current situation of Meydan-ı Şerif and the Meydan-ı Şerif room (photo taken by author).</p>
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<p>Exterior (<b>left</b>) and interior (<b>right</b>) view of the Matbah-ı Şerif that is used as a museum after reconstruction (photo taken by author).</p>
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<p>Photographs taken from inside and outside the tomb (Old photos: [<a href="#B41-buildings-15-00568" class="html-bibr">41</a>]; New photos: photo taken by author).</p>
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<p>Tomb, Dedegan Rooms, Selamlık, and Fountain (Old photo: [<a href="#B50-buildings-15-00568" class="html-bibr">50</a>]; New Photo: (photo taken by author).</p>
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<p>State of the Selamlık section before demolition [<a href="#B41-buildings-15-00568" class="html-bibr">41</a>] and after reconstruction (photo taken by author).</p>
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<p>The photos of the southern facade of the Selamlık facing Bayramyeri Street (photo taken by author).</p>
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<p>Dedegan rooms before demolition [<a href="#B41-buildings-15-00568" class="html-bibr">41</a>] and after reconstruction (photo taken by author).</p>
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<p>Fountain in the courtyard before demolition [<a href="#B41-buildings-15-00568" class="html-bibr">41</a>] and after reconstruction (photo taken by author).</p>
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<p>Site plan analysis of the Bursa Mevlevi Lodge before and after reconstruction (created by authors).</p>
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<p>Functional analysis of the Bursa Mevlevi Lodge before and after reconstruction (created by authors).</p>
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<p>A comparative analysis of architectural and facade characteristics of the Bursa Mevlevi Lodge after reconstruction (created by authors).</p>
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13 pages, 7948 KiB  
Article
Fatigue Resistance Improvement in Cold-Drawn NiTi Wires Treated with ALD: A Preliminary Investigation
by David Vokoun, Ondřej Tyc, Sneha Manjaree Samal, Ivo Stachiv, Yoshane Yu and Chichung Kei
Appl. Sci. 2025, 15(4), 1823; https://doi.org/10.3390/app15041823 - 11 Feb 2025
Abstract
NiTi shape memory alloys (SMAs) are widely studied for their potential applications, and atomic layer deposition (ALD) is an effective technique for coating them due to its precise control over coating thickness. This study investigates the impact of Al2O3 coating [...] Read more.
NiTi shape memory alloys (SMAs) are widely studied for their potential applications, and atomic layer deposition (ALD) is an effective technique for coating them due to its precise control over coating thickness. This study investigates the impact of Al2O3 coating on the fatigue behavior of cold-drawn NiTi wires with a 0.125 mm diameter. The wires were coated using atomic layer deposition (ALD) with 100 ALD cycles. Fatigue tests were conducted in tensile mode at room temperature, applying cyclic loading between 0–50, and 700 MPa (700 MPa is almost 40% of ultimate tensile strength). The results show that the cold-drawn NiTi wires failed after an average of 7500 tensile loading cycles, while the lifetime of the coated and stretched NiTi wires with a preload of 1.7–2.8 kg significantly improved, with an average of 293,000 cycles before failure. Full article
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<p>The schematics of the ALD chamber with the stretched-wire sample placed inside the chamber.</p>
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<p>The schematics for the idea of building compressive stress at the wire surface using ALD to fill microcracks with Al<sub>2</sub>O<sub>3</sub>.</p>
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<p>The SEM micrographs of the surface of the uncoated-NiTi-wire sample using secondary electron (SE) (<b>a</b>) and back-scatter electron (BSE) (<b>b</b>) detectors and coated-NiTi-wire sample (100 Al<sub>2</sub>O<sub>3</sub> ALD cycles) using SE (<b>c</b>) and BSE (<b>d</b>) detectors. The magnification and acceleration voltage were 10.0k× and 5 kV, respectively. The white arrows in the SEM images indicate microcracks.</p>
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<p>Energy-dispersive X-ray spectrum from the (<b>a</b>) as-purchased and the (<b>b</b>) coated-NiTi-wire sample. Accelerating voltage and counting time were 5 kV and 100 s, respectively.</p>
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<p>The stress—strain diagrams until the fracture at room temperature for the individual noncoated samples (<b>a</b>–<b>f</b>).</p>
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<p>The stress—strain diagrams until the fracture at room temperature for the individual ALD-coated samples (<b>a</b>–<b>e</b>) and the electrical resistance—number of loading cycles diagram (<b>f</b>) for NiTi wire sample ALD_wire_3.</p>
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<p>HAADF (high-angle annular dark field) image of a thin lamella cut parallel to the wire axis and the radial direction (<b>a</b>,<b>b</b>). The atomic content (at.%) of selected chemical elements (<b>c</b>) along the orange line shown in panel (<b>b</b>).</p>
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<p>The comparison of the tensile loading curves of the as-purchased and ALD-coated wires (under load of 2.8 kg) loaded until the fracture.</p>
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30 pages, 2090 KiB  
Article
Ubunye: An MEC Orchestration Service Based on QoE, QoS, and Service Classification Using Machine Learning
by Kilbert Amorim Maciel, David Martins Leite, Guilherme Alves de Araújo, Flavia C. Delicato and Atslands R. Rocha
Future Internet 2025, 17(2), 66; https://doi.org/10.3390/fi17020066 - 5 Feb 2025
Abstract
The increasing adoption of Internet of Things devices has led to a significant demand for cloud services, where latency and bandwidth play a crucial role in shaping users’ perception of network service quality. However, the use of cloud services with the desired quality [...] Read more.
The increasing adoption of Internet of Things devices has led to a significant demand for cloud services, where latency and bandwidth play a crucial role in shaping users’ perception of network service quality. However, the use of cloud services with the desired quality is not always available to all users. Furthermore, uneven network coverage in urban and rural areas has created “digital deserts”, which are characterized by a lack of connectivity resources, complicating access to cloud services. In this scenario, edge computing emerges as a promising alternative for service provision. Edge computing leverages data processing at or near the source where it is generated rather than sending it to the cloud for processing. It can lead to several advantages, such as reduced latency and lower bandwidth usage. This paper addresses the need to ensure consistent quality of experience (QoE) and quality of service (QoS) in dynamic network environments, particularly in remote regions with limited infrastructure. We propose an orchestration service called Ubunye, which operates at the network edge and selects the most appropriate edge node to fulfill a given application request while satisfying its quality requirements. Ubunye considers factors such as latency and available bandwidth when selecting a node to execute the requested service. It implements a service classification system based on machine learning (ML) techniques. The ideal edge node is chosen through a multi-faceted evaluation, which includes current CPU load, memory availability, and other relevant parameters. Experiment results show that Ubunye effectively orchestrates resources at the network edge, enhancing QoE and QoS for services that demand low latency and high bandwidth. Additionally, it showcases the ability to classify services and allocate resources under challenging network conditions. Full article
(This article belongs to the Special Issue Internet of Things Technology and Service Computing)
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<p>Ubunye architecture’s operational process.</p>
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<p>Ubunye service classification.</p>
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<p>Ubunye service classification—correlation matrix.</p>
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<p>Ubunye latency algorithm.</p>
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<p>Ubunye BW algorithm.</p>
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<p>Stopping criterion and simulation execution.</p>
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<p>Ubunye service classification – confusion matrix.</p>
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<p>Ubunye service components using the EdgeSimPy simulator.</p>
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<p>Mean user delay (in milliseconds): the ratio between the sum of the delays of all user requests and the total number of requests, varying the number of users in each scenario.</p>
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<p>Total user delay (in seconds): the total sum of user delay over the total simulation time, varying the number of users in each scenario.</p>
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<p>Mean bandwidth available (in megabits per second): measured in the first ten minutes of the simulation for the 150-user scenario.</p>
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<p>Consumption of CPU resources: percentage of the total CPU consumption for five algorithms, varying the number of users in each scenario.</p>
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<p>Memory usage: the percentage of memory used by the five algorithms varies by the number of users in each scenario.</p>
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<p>User request success rate: percentage ratio between successfully answered user requests and the total number of user requests during the simulation in each scenario.</p>
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<p>Mean user delay (in milliseconds): the ratio between the sum of the delays of all user requests and the total number of requests, varying the number of users in each faulty scenario.</p>
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<p>Total user delay (in seconds): the total sum of user delay over the total simulation time, varying the number of users in each faulty scenario.</p>
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<p>Mean bandwidth available on the faulty scenario (in megabits per second): measured in the first ten minutes of the simulation for the 150-user scenario.</p>
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<p>Consumption of CPU resources: percentage of the total CPU consumption for the five algorithms, varying the number of users in each faulty scenario.</p>
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<p>Memory usage: the percentage of memory used by the five algorithms varies by the number of users in each faulty scenario.</p>
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<p>User request success rate: percentage ratio between successfully answered user requests and the total number of user requests during the simulation in each faulty scenario.</p>
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<p>Summary: the average of each performance metric was calculated, and the highest metric was used as a benchmark.</p>
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25 pages, 9363 KiB  
Article
Globalization and Architecture: Urban Homogenization and Challenges for Unprotected Heritage. The Case of Postmodern Buildings with Complex Geometric Shapes in the Ensanche of San Sebastián
by María Senderos, Maialen Sagarna, Juan Pedro Otaduy and Fernando Mora
Buildings 2025, 15(3), 497; https://doi.org/10.3390/buildings15030497 - 5 Feb 2025
Abstract
Globalization has profoundly impacted architecture by promoting urban homogenization, where global styles and materials overshadow local character. This shift prioritizes standardized functionality and energy efficiency over cultural identity, erasing regional architectural distinctiveness. In historical urban centers, globalization-driven interventions—such as ventilated facades or external [...] Read more.
Globalization has profoundly impacted architecture by promoting urban homogenization, where global styles and materials overshadow local character. This shift prioritizes standardized functionality and energy efficiency over cultural identity, erasing regional architectural distinctiveness. In historical urban centers, globalization-driven interventions—such as ventilated facades or external thermal insulation systems (ETISs)—often simplify original compositions and alter building materiality, texture, and color. The Ensanche of San Sebastián serves as a case study highlighting this issue. Despite its architectural richness, which includes neoclassical and modernist buildings primarily constructed with sandstone from the Igeldo quarry, unprotected buildings are at risk of unsympathetic renovations. Such changes can distort the identity of what is considered “everyday heritage”, encompassing the residential buildings and public spaces that shape the collective memory of cities. This study presents a replicable methodology for assessing the vulnerability of buildings to facade interventions. By utilizing tools like digital twins, point cloud modeling, and typological analysis, the research establishes criteria for interventions aimed at preserving architectural values. It emphasizes the importance of collaborative efforts with urban planning authorities and public awareness campaigns to safeguard heritage. Ultimately, protecting architectural identity requires balancing the goals of energy efficiency with cultural preservation. This approach ensures that urban landscapes maintain their historical and social significance amidst globalization pressures. Full article
(This article belongs to the Special Issue Selected Papers from the REHABEND 2024 Congress)
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<p>DSRM simplified flow diagram.</p>
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<p>Buildings in the Ensanche of San Sebastián classified as stone sculptures.</p>
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<p>Site plan with the unprotected buildings of the Ensanche, the postmodern buildings with unique volumetry, and the San Martín 37 building.</p>
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<p>Photograph of the building located on Marina 8 street, prior to facade intervention (2013) and post-intervention (2022). Source: Google Maps.</p>
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<p>Building front of the odd numbers of C/San Martín. Case study building located at number 37, framed in a red rectangle. Restitution obtained with the free software Hugin (Hugin 2022.0.0).</p>
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<p>Number of unprotected buildings in the Ensanche classified by scenario.</p>
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<p>Characterization sheet of a building in the stage and sub-scenario and evaluation sheet of the vulnerability of a building in the stage and sub-scenario of a stone sculptural building.</p>
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<p>Scanning points at the intersection between Easo and San Martín streets and point cloud obtained for the survey of the facade of 37 San Martín Street.</p>
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<p>Model of the current state of the facade of the case study in Revit software and rendered image with finishes and textures.</p>
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<p>Simulation of a possible intervention of the envelope with the substitution of material and color and simplification of the geometry; cladding detail on the front of the curved balcony and replacement of metal railings with translucent glass.</p>
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<p>Simulations performed from the image on the left in different AI software (top Archivinci (Cigraph, Milan, Italy), middle Copilot (Microsoft 365 Copilot, 2025), and bottom PromeAI (PromeAI, 2025)).</p>
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<p>The sheet used to establish the specific intervention criteria for this building.</p>
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<p>The sheet used to establish the specific intervention criteria for this building.</p>
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<p>@ck_armin social media account in Instagram.</p>
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15 pages, 270 KiB  
Article
Literary Tourism and Cultural Sustainability: The Landscape of Beppe Fenoglio in the Langhe, Italy
by Giovanna Rech, Chiara Pini, Lorenzo Migliorati and Luca Mori
Sustainability 2025, 17(3), 1237; https://doi.org/10.3390/su17031237 - 4 Feb 2025
Abstract
This article explores the niche sector of literary tourism with a focus on the works of Italian writer Beppe Fenoglio in the Langhe-Roero and Monferrato area of Piedmont, Italy. It questions whether literary tourism can contribute to the cultural sustainability of a landscape. [...] Read more.
This article explores the niche sector of literary tourism with a focus on the works of Italian writer Beppe Fenoglio in the Langhe-Roero and Monferrato area of Piedmont, Italy. It questions whether literary tourism can contribute to the cultural sustainability of a landscape. Nowadays, this area is already a well-established tourist destination known for its food and wine; however, Fenoglio’s work offers a different perspective, highlighting a specific heritage comprising the area’s rural life, local culture, and history of the Resistance movement. The research used a mixed method approach with documentary analysis, questionnaires, and in-depth interviews. “Fenoglians” (tourists motivated by Fenoglio’s life and works) were identified, and their characteristics were explored. The results cannot be generalized, as the chosen sampling method does not provide sufficient materials for broad application. While being a small group, these special interest tourists represent an opportunity for tourism diversification. This article concludes that Fenoglio’s literary tourism offers a distinctive experience, fosters new interpretations of the landscape, and strengthens collective memory of the Resistance. It highlights the importance of local communities in understanding how fictional narratives shape tourist perceptions of a destination as well as their role in preserving the community’s collective memory and landscape. Full article
(This article belongs to the Special Issue Culture, Landscape and Sustainability)
15 pages, 4052 KiB  
Article
Viscoelastic, Shape Memory, and Fracture Characteristics of 3D-Printed Photosensitive Epoxy-Based Resin Under the Effect of Hydrothermal Ageing
by Mohamad Alsaadi, Tamer A Sebaey, Eoin P. Hinchy, Conor T. McCarthy, Tielidy A. de M. de Lima, Alexandre Portela and Declan M. Devine
J. Manuf. Mater. Process. 2025, 9(2), 46; https://doi.org/10.3390/jmmp9020046 - 1 Feb 2025
Abstract
Using 3D-printed (3DPd) polymers and their composites as shape memory materials in various smart engineering applications has raised the demand for such functionally graded sustainable materials. This study aims to investigate the viscoelastic, shape memory, and fracture toughness properties of the epoxy-based ultraviolet [...] Read more.
Using 3D-printed (3DPd) polymers and their composites as shape memory materials in various smart engineering applications has raised the demand for such functionally graded sustainable materials. This study aims to investigate the viscoelastic, shape memory, and fracture toughness properties of the epoxy-based ultraviolet (UV)-curable resin. A UV-based DLP (Digital Light Processing) printer was employed for the 3D printing (3DPg) epoxy-based structures. The effect of the hydrothermal accelerated ageing on the various properties of the 3DPd components was examined. The viscoelastic performance in terms of glass transition temperature (Tg), storage modulus, and loss modulus was evaluated. The shape memory polymer (SMP) performance with respect to shape recovery and shape fixity (programming the shape) were calculated through dynamic mechanical thermal analysis (DMTA). DMTA is used to reveal the molecular mobility performance through three different regions, i.e., glass region, glass transition region, and rubbery region. The shape-changing region (within the glass transition region) between the Tg value from the loss modulus and the Tg value from the tan(δ) was analysed. The temperature memory behaviour was investigated for flat and circular 3DPd structures to achieve sequential deployment. The critical stress intensity factor values of the single-edge notch bending (SENB) specimens have been explored for different crack inclination angles to investigate mode I (opening) and mixed-mode I/III (opening and tearing) fracture toughness. This study can contribute to the development of highly complex shape memory 3DPd structures that can be reshaped several times with large deformation. Full article
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<p>Schematic diagram of the thermomechanical SMP cycle [<a href="#B4-jmmp-09-00046" class="html-bibr">4</a>].</p>
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<p>The programming/recovery process: (<b>a</b>) schematic diagram and (<b>b</b>) images of the 3DPd specimens under the programming/recovery process.</p>
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<p>Schematic diagram of the geometrical configuration of the SENB specimen.</p>
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<p>(<b>a</b>) DSC analysis before and after thermal post-curing; (<b>b</b>) the change in water uptake versus ageing time of the 3DP-Ep objects.</p>
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<p>Viscoelastic properties of the 3DP-Ep before and after the hydrothermal ageing: (<b>a</b>) <span class="html-italic">E’</span>, (<b>b</b>) (<span class="html-italic">tan(δ)</span>), and (<b>c</b>) <span class="html-italic">E</span>”.</p>
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<p>Thermomechanical SMP cycle of 3DPd samples using 4-step DMTA test, (<b>a</b>) Ep-135 °C, Ep-170 °C and Me-100 °C samples, (<b>b</b>) EP0h, EP600h, and EP1800 h samples.</p>
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<p>3DPd epoxy-based structures demonstrate temporary and recovery shapes.</p>
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<p>Mode I and mixed mode I/III critical stress intensity factors of the 3DP-Ep beams.</p>
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<p>(<b>i</b>) SENB specimens under test, and (<b>ii</b>) the samples and fracture surfaces of the (<b>a</b>) mode I θ = 90°, (<b>b</b>) mixed-mode I/III θ = 60°, and (<b>c</b>) mixed-mode I/III θ = 30°.</p>
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<p>SEM micrographs of the tensile test specimen fracture surface (red frame represents the location of the 50 µ image).</p>
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21 pages, 11288 KiB  
Article
Impact of NiTi Shape Memory Alloy Substrate Phase Transitions Induced by Extreme Temperature Variations on the Tribological Properties of TiN Thin Films
by Mingxi Hou, Dong Xie, Xiaoting Wang, Min Guan, Diqi Ren, Yongyao Su, Donglin Ma and Yongxiang Leng
Coatings 2025, 15(2), 155; https://doi.org/10.3390/coatings15020155 - 1 Feb 2025
Abstract
NiTi alloys and thin film/NiTi composites are extensively utilized in frictional environments, particularly those experiencing extreme temperature fluctuations. Current studies mainly focus on preparing wear-resistant films on NiTi alloy surfaces but neglect the potential impact of temperature-induced phase transitions in the NiTi substrate [...] Read more.
NiTi alloys and thin film/NiTi composites are extensively utilized in frictional environments, particularly those experiencing extreme temperature fluctuations. Current studies mainly focus on preparing wear-resistant films on NiTi alloy surfaces but neglect the potential impact of temperature-induced phase transitions in the NiTi substrate on thin films’ performance. This study examines the effect of NiTi alloy phase transitions, induced by extreme temperature variations, on the tribological properties of TiN thin films on NiTi substrates. TiN films (1 μm thick) were deposited on NiTi alloy surfaces using magnetron sputtering technology. The transition of the main phase in the NiTi substrate between the R phase and the B19′ phase was achieved via liquid nitrogen cooling (−196 °C) and water bath heating (90 °C). XRD, EDS, SEM, and tribological tests analyzed the phase structure, elemental composition, micromorphology, and tribological behavior. Fatigue wear was identified as the predominant wear mechanism for the TiN films, with minor contributions from oxidative and abrasive wear. Phase transition from the R phase to the B19′ phase in the NiTi substrate induced by temperature change couls reduce the wear rate of the TiN film by up to 41.97% and decrease the friction coefficient from about 0.45 to about 0.25. Furthermore, the shape memory effect of the NiTi alloy substrate, caused by B19′ → B2 phase transition, resulted in the recovery of the TiN thin film wear track depth from 920 nm to 550 nm, manifesting a “self-healing” phenomenon. The results in this study are important and necessary for the provision of thin film/NiTi composites in frictional environments. Full article
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<p>Experimental flow diagram.</p>
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<p>TiN thin film microstructure and EDS mapping: (<b>a</b>) TiN/Si cross-section; (<b>b</b>) TiN/Si surface; (<b>c</b>) TiN/NiTi surface; (<b>d</b>) TiN/304 surface; and (<b>e</b>) EDS of TiN/Si.</p>
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<p>TiN thin film microstructure and EDS mapping: (<b>a</b>) TiN/Si cross-section; (<b>b</b>) TiN/Si surface; (<b>c</b>) TiN/NiTi surface; (<b>d</b>) TiN/304 surface; and (<b>e</b>) EDS of TiN/Si.</p>
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<p>XRD pattern of (<b>a</b>) TiN/NiTi alloy and (<b>b</b>) TiN/304 stainless steel.</p>
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<p>(<b>a</b>) TiN/NiTi wear scar SEM; (<b>b</b>) TiN/NiTi wear scar EDS; (<b>c</b>) TiN/304 wear scar SEM; and (<b>d</b>) TiN/304 wear scar EDS.</p>
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<p>(<b>a</b>) TiN/NiTi wear scar SEM; (<b>b</b>) TiN/NiTi wear scar EDS; (<b>c</b>) TiN/304 wear scar SEM; and (<b>d</b>) TiN/304 wear scar EDS.</p>
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<p>Wear characteristics of TiN film on NiTi alloy substrate: (<b>a</b>) SEM image of the inside of the wear scar; (<b>b</b>) EDS of friction debris; (<b>c</b>) defects in the wear scar: (①) defect ①, (②) defect ②, (③) defect ③; and (<b>d</b>) EDS corresponding to defect ①.</p>
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<p>Wear rates of NiTi alloy, TiN/NiTi, 304 stainless steel, and TiN/304.</p>
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<p>Effect of cryogenic–thermal cycle treatment on the wear rate of two composites: (<b>a</b>) TiN/NiTi and (<b>b</b>) TiN/304.</p>
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<p>Changes in the wear scar profile of two composites during the first cryogenic–thermal cycle: (<b>a</b>) TiN/NiTi and (<b>b</b>) TiN/304.</p>
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<p>The change in friction coefficient of composites during the first cryogenic–thermal cycle: (<b>a</b>) TiN/NiT and (<b>b</b>) TiN/304.</p>
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<p>Changes in wear rate of the first wear scar on (<b>a</b>) TiN/NiTi and (<b>b</b>) TiN/304.</p>
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<p>Changes in the outline of the first wear scar on (<b>a</b>) TiN/NiTi and (<b>b</b>) TiN/304.</p>
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<p>The morphologies at the tail of the first wear scar on two composite materials during the first cryogenic–thermal cycle: (<b>a</b>) initial TiN/NiTi; (<b>b</b>) TiN/NiTi after cryogenic treatment; (<b>c</b>) TiN/NiTi after cryogenic–thermal treatment; (<b>d</b>) initial TiN/304; (<b>e</b>) TiN/304 after cryogenic treatment; and (<b>f</b>) TiN/304 after cryogenic–thermal treatment.</p>
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16 pages, 4047 KiB  
Article
Long-Term Immune Consequences of Initial SARS-CoV-2 A.23.1 Exposure: A Longitudinal Study of Antibody Responses and Cross-Neutralization in a Ugandan Cohort
by Gerald Kevin Oluka, Jackson Sembera, Joseph Ssebwana Katende, Violet Ankunda, Laban Kato, Ashwini Kurshan, Carl Graham, Jeffrey Seow, Katie J. Doores, Michael H. Malim, Julie M. Fox, Pontiano Kaleebu and Jennifer Serwanga
Vaccines 2025, 13(2), 143; https://doi.org/10.3390/vaccines13020143 - 29 Jan 2025
Abstract
Background: This study assessed the long-term dynamics of neutralizing antibodies in a Ugandan cohort primarily exposed to the A.23.1 SARS-CoV-2 variant, examining how this shaped immune breadth and potency against diverse strains following infection and prototype-based vaccination. Methods: We conducted a 427-day retrospective [...] Read more.
Background: This study assessed the long-term dynamics of neutralizing antibodies in a Ugandan cohort primarily exposed to the A.23.1 SARS-CoV-2 variant, examining how this shaped immune breadth and potency against diverse strains following infection and prototype-based vaccination. Methods: We conducted a 427-day retrospective analysis of 41 participants across multiple SARS-CoV-2 waves, assessing binding and neutralizing antibody responses using in-house ELISA and pseudotyped virus neutralization assays. We quantified immune responses to key SARS-CoV-2 variants, A.23.1, D614G, Delta, and BA.4, capturing evolving immunity across the pandemic. Results: Neutralizing antibody titers against A.23.1 remained significantly higher than those against D614G, Delta, and BA.4, highlighting the solid immune memory following A.23.1 infection. Consistently lower titers were observed for BA.4 across all time points, aligning with its strong immune-evasion capability. Correlations between neutralizing titers and spike-directed IgG (S-IgG) concentrations were significantly stronger for A.23.1 than for D614G, with no correlation for BA.4. ChAdOx1-S vaccination substantially elevated the neutralizing titers across all variants, most notably BA.4, highlighting the essential role of vaccination in boosting immunity, even in individuals with initially low titers. Conclusions: Initial exposure to the A.23.1 variant triggered potent immune responses, shaping neutralizing antibody dynamics during subsequent exposures. These findings highlight the importance of accounting for early viral exposures in vaccine development and public health planning. The distinctly lower immune response to BA.4 highlights the need for continuous antigenic monitoring and timely vaccine updates for protection against emerging variants. Vaccination remains essential for reinforcing and sustaining immunity against evolving variants. Full article
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<p>COVID-19 variant distribution and participant baseline characteristics. This figure shows the timeline of daily COVID-19 case counts and variant distribution from March 2020 to February 2022, indicating that samples collected between July 2020 and October 2021 are primarily linked to the A.23.1 and Delta variants. This figure is adapted and reused with permission from Bbosa et al. [<a href="#B21-vaccines-13-00143" class="html-bibr">21</a>].</p>
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<p>Longitudinal comparison of neutralizing titers and S-IgG levels across SARS-CoV-2 strains. This figure illustrates the longitudinal trends in neutralizing antibody titers and full spike (S)-IgG concentrations across SARS-CoV-2 variants. The line plots show neutralization titers over time for the D614G prototype and the A.23.1, Delta, and BA.4 variants, with the time categorized into four quarterly intervals, 0–91, 92–182, 183–273, and 274–427 days (<b>A</b>), and the median titers per quarter (<b>B</b>). Boxplots illustrate the distributions of antibody levels displaying medians (horizontal black line) and interquartile ranges (top and bottom of the box) across study groups. Boxplots depict the distribution of neutralizing titers for each virus variant across quarterly time intervals (<b>C</b>). Additionally, comparative boxplots illustrate S-IgG concentrations (ng/mL) across the D614G prototype and the A.23.1 variants, analyzed for all study participants (<b>D</b>). Using the D614G S-IgG cut-off of 0.432, the data were further stratified by D614G responders and non-responders at each quarterly time point (<b>E</b>). Statistical significance was determined at a threshold of <span class="html-italic">p</span> ≤ 0.05. Significance bars indicate the <span class="html-italic">p</span>-values.</p>
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<p>Longitudinal potency and breadth of neutralizing antibody responses against SARS-CoV-2 variants over 427 days. This figure shows a heatmap and bar graph illustrating the neutralizing antibody responses against various SARS-CoV-2 variants over 427 days. In the heatmap (<b>A</b>), darker cells represent higher neutralizing titers, while lighter cells indicate lower titers; white cells represent missing data. Each row corresponds to a participant’s neutralization responses over time, highlighting that only a few participants maintained high neutralizing titers across all viruses and time points. The stacked bar graph (<b>B</b>) shows the proportion of participants within different neutralization titer groups over time for each variant. Most subjects displayed low (25–100) titers against D614G, intermediate (100–500) titers against A.23.1, and a mix of low and intermediate titers against the Delta variant.</p>
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<p>Correlation heat map of neutralizing antibody titers against SARS-CoV-2 variants and spike-directed IgG antibodies. This figure displays heat maps comparing the correlations between neutralizing antibody titers against SARS-CoV-2 variants D614G, A.23.1, Delta, and BA.4 and spike-directed IgG antibody levels for D614G (<b>A</b>) and A.23.1 (<b>B</b>). Positive correlations are indicated in purple, while negative correlations are shown in red. Statistical significance was determined at a threshold of <span class="html-italic">p</span> ≤ 0.05; <span class="html-italic">p</span>-values are indicated in the heatmap.</p>
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<p>Fold changes in neutralizing titers relative to D614G and A.23.1 and neutralization patterns in re-infected and vaccinated Subjects. This figure shows the log-transformed geometric mean titer (GMT) fold changes in neutralizing antibody responses relative to D614G (<b>A</b>) and A.23.1 (<b>B</b>) across different time points in a cohort of 41 participants. A fold change above 0 indicates an increase, while a fold change below 0 indicates a decrease in neutralizing titers relative to the reference virus. Panel (<b>C</b>) displays the neutralizing titers of re-infected subjects over time, categorized by days post-infection, with a focus on variations in neutralization responses across different virus variants. (<b>D</b>) illustrates the neutralizing titers before and after vaccination in vaccinated subjects, showing the comparative changes in responses to each virus variant following vaccination. Horizontal lines represent the log-transformed geometric mean titers at each time point for each virus. Fold changes are presented as log-transformed values, with raw unlogged values in brackets. Statistically significant differences are indicated, marked by <span class="html-italic">p</span>-values ≤ 0.05, confirming a consistent rise in antibody titers across all variants following vaccination.</p>
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14 pages, 29079 KiB  
Article
Molecular Dynamics Investigation on Grain Size-Dependent Superelastic Behavior of CuZr Shape Memory Alloys
by Mixun Zhu, Kai Wang, Hongtao Zhong, Huahuai Shen, Yong Zhang, Xiaoling Fu and Yuanzheng Yang
Metals 2025, 15(2), 142; https://doi.org/10.3390/met15020142 - 29 Jan 2025
Abstract
The superelasticity of CuZr shape memory alloys (SMAs) originates from stress-induced transformations between the B2 (austenite) and B19’ (martensite) phases. Grain size is a key parameter affecting the superelasticity of shape memory alloys. Previous studies on NiTi, Fe-based, and Cu-based SMAs confirm that [...] Read more.
The superelasticity of CuZr shape memory alloys (SMAs) originates from stress-induced transformations between the B2 (austenite) and B19’ (martensite) phases. Grain size is a key parameter affecting the superelasticity of shape memory alloys. Previous studies on NiTi, Fe-based, and Cu-based SMAs confirm that altering grain size effectively regulates superelasticity. Current research on the influence of grain size on the superelasticity of CuZr shape memory alloys (SMAs) is relatively sparse. This study employs molecular dynamics simulations to evaluate the effect of grain size on the superelasticity of CuZr SMAs through uniaxial loading–unloading tests. Polycrystalline samples with grain sizes of 6.59 nm, 5 nm, and 4 nm were analyzed. The results indicate that reducing grain size can decrease the irrecoverable strain, thereby enhancing superelasticity. The improvement in superelasticity is attributed to a higher recovery rate of the martensite-to-austenite transformation, allowing more plastic deformation within the grain interior to recover during unloading, and thereby reducing the irrecoverable strain. The recovery rate of the martensite-to-austenite transformation is closely related to the elastic strain energy accumulated within the grain interior during loading. Full article
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Figure 1
<p>Polycrystalline B2-CuZr samples with different average grain sizes of (<b>a</b>) <span class="html-italic">d</span><sub>ave</sub> = 6.59 nm, (<b>b</b>) <span class="html-italic">d</span><sub>ave</sub> = 5 nm, and (<b>c</b>) <span class="html-italic">d</span><sub>ave</sub> = 4 nm. The B2-CuZr crystals within the grain interior are colored in blue and the grain boundaries are colored in white.</p>
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<p>Engineering stress–strain curves of polycrystalline B2-CuZr samples with grain sizes of 6.59 nm, 5 nm, and 4 nm during tensile loading and unloading.</p>
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<p>The evolution of local shear strain distribution and the corresponding phase configuration in polycrystalline B2-CuZr samples with grain sizes of (<b>a</b>) 6.59 nm, (<b>b</b>) 5 nm, and (<b>c</b>) 4 nm. The initial state without applied strain (<span class="html-italic">ε</span> = 0), the critical strain for martensitic transformation, the maximum strain of loading (<span class="html-italic">ε</span> = 0.08), and the end point of unloading were selected for display.</p>
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<p>Phase content evolution of polycrystalline B2-CuZr samples with grain sizes of (<b>a</b>) 6.59 nm, (<b>b</b>) 5 nm, and (<b>c</b>) 4 nm during loading and unloading.</p>
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<p>(<b>a</b>) The volumetric strain <math display="inline"><semantics> <mrow> <msub> <mi>ε</mi> <mi mathvariant="normal">V</mi> </msub> </mrow> </semantics></math> and irrecoverable strain of polycrystalline B2-CuZr samples with different grain sizes. (<b>b</b>) The volumetric strain <math display="inline"><semantics> <mrow> <msub> <mi>ε</mi> <mi mathvariant="normal">V</mi> </msub> </mrow> </semantics></math> of polycrystal, grain interior, and grain boundaries with different grain sizes.</p>
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<p>The engineering stress–strain curves of polycrystalline B2-CuZr samples with grain sizes of (<b>a</b>) 6.59 nm, (<b>b</b>) 5 nm, and (<b>c</b>) 4 nm and the corresponding potential energy changes with applied strain.</p>
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<p>The correlation between the recovery rate of the R phase and the elastic energy accumulation within the grain interior during loading.</p>
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13 pages, 4412 KiB  
Article
Acoustic Emission During Rubber-like Deformation in Ni51Fe18Ga27Co4 Single Crystalline Shape Memory Alloys
by Lajos Daróczi, Sarah M. Kamel, László Z. Tóth, Elena Yu. Panchenko, Yuri I. Chumljakov and Dezső L. Beke
Metals 2025, 15(2), 131; https://doi.org/10.3390/met15020131 - 28 Jan 2025
Abstract
Acoustic emission, AE, belonging to a rubber-like deformation in a martensitic state after the stabilization aging of the stress-induced martensite (SIM aging) of Ni51Fe18Ga27Co4 single crystals in compression, were investigated. AE activity in the plateau regions [...] Read more.
Acoustic emission, AE, belonging to a rubber-like deformation in a martensitic state after the stabilization aging of the stress-induced martensite (SIM aging) of Ni51Fe18Ga27Co4 single crystals in compression, were investigated. AE activity in the plateau regions of the stress–strain loop is due to a massive reorientation from the variants produced by SIM aging to the variants preferred by the compressive stress (perpendicular to the stress used in SIM aging) and vice versa. For unloading, the large AE activity just at the knee point of the stress–stain curve is attributed to the difficulty of the re-nucleation of the SIM aging-stabilized martensite variant. The amplitude, peak energy, and area of signals can be described by power-like distributions and the characteristic exponents are in good agreement with data obtained in other alloys. Power law cross-correlations between the energy, E, and amplitude, A, as well as between the area, S, and the amplitude, A, were also analyzed. It was found that the exponents are given by 3φ as well as 2φ, respectively, with φ0.7. Normalized universal temporal shapes of avalanches (i.e., the UA  versus tA1φ plots, where U is the detected voltage) for a fixed area scale very well together. The tail of the normalized temporal shape decays more slowly than the theoretical prediction, which can be attributed to an intrinsic absorption of AE signals and/or to the overlap of sub-avalanches. Full article
(This article belongs to the Special Issue Metallic Functional Materials: Development and Applications)
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<p>Schematic picture of the measuring setup. The arrow shows the sample and the box at the top anvil is the sensor.</p>
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<p>(<b>a</b>) Compression stress–strain curve; (<b>b</b>) stress (black), energy of acoustic emission signals (red), and the cumulative AE energy, <math display="inline"><semantics> <mrow> <mrow> <mo stretchy="false">∑</mo> <mrow> <mi mathvariant="bold-italic">E</mi> </mrow> </mrow> </mrow> </semantics></math>, (blue) as a function of time (taken with a 1.25 × 10<sup>−3</sup> s<sup>−1</sup> strain rate). A large acoustic activity and large jump in <math display="inline"><semantics> <mrow> <mrow> <mo stretchy="false">∑</mo> <mrow> <mi mathvariant="bold-italic">E</mi> </mrow> </mrow> </mrow> </semantics></math> can be observed on the unloading curve.</p>
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<p>The energy probability distribution density function of acoustic signals obtained during rubber-like deformation (<b>a</b>). (<b>b</b>) The maximum likelihood fit for the exponent.</p>
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<p><span class="html-italic">LogE</span> versus <span class="html-italic">LogA</span>. The insert shows the slope of the straight line fitted.</p>
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<p><span class="html-italic">LogS</span> versus <span class="html-italic">LogA</span>. The insert shows the slope of the straight line fitted.</p>
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<p>An optical micrograph of the martensite structure: (<b>a</b>) original, V1, state with a dominantly de-twinned region, with minor residual twins; (<b>b</b>) twinned, reoriented, V2/V3, martensite; and (<b>c</b>) the final state, which is equivalent to the initial state.</p>
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<p>Averaged AE signals in different size (area) ranges (the insert gives the center values of S within which the averaging was made).</p>
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<p>Averaged AE signals after a normalization of the vertical and horizontal axes by A<sub>m</sub> and A<sub>m</sub><sup>1−φ</sup>, respectively.</p>
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<p>Fitting the exponentially decaying tail of the curve on <a href="#metals-15-00131-f010" class="html-fig">Figure 10</a> (<math display="inline"><semantics> <mrow> <msup> <mrow> <mi>U</mi> </mrow> <mrow> <mi>*</mi> </mrow> </msup> <mo>=</mo> <mstyle scriptlevel="0" displaystyle="true"> <mfrac> <mrow> <mi>U</mi> </mrow> <mrow> <mi>A</mi> </mrow> </mfrac> </mstyle> <mtext> </mtext> </mrow> </semantics></math> and <math display="inline"><semantics> <mrow> <msup> <mrow> <mi>t</mi> </mrow> <mrow> <mi>*</mi> </mrow> </msup> <mo>=</mo> <mstyle scriptlevel="0" displaystyle="true"> <mfrac> <mrow> <mi>t</mi> </mrow> <mrow> <msup> <mrow> <mi>A</mi> </mrow> <mrow> <mn>1</mn> <mo>−</mo> <mi>φ</mi> </mrow> </msup> </mrow> </mfrac> </mstyle> </mrow> </semantics></math>): according to Equation (2) (<b>a</b>) as well as by <math display="inline"><semantics> <mrow> <mo>~</mo> <msup> <mrow> <mi>e</mi> </mrow> <mrow> <mo>−</mo> <mstyle scriptlevel="0" displaystyle="true"> <mfrac> <mrow> <mi>t</mi> </mrow> <mrow> <msub> <mrow> <mi>τ</mi> </mrow> <mrow> <mi>a</mi> </mrow> </msub> </mrow> </mfrac> </mstyle> </mrow> </msup> </mrow> </semantics></math> type function (<b>b</b>). It can be seen that the fit <math display="inline"><semantics> <mrow> <mo>~</mo> <msup> <mrow> <mi>e</mi> </mrow> <mrow> <mo>−</mo> <mstyle scriptlevel="0" displaystyle="true"> <mfrac> <mrow> <mi>t</mi> </mrow> <mrow> <msub> <mrow> <mi>τ</mi> </mrow> <mrow> <mi>a</mi> </mrow> </msub> </mrow> </mfrac> </mstyle> </mrow> </msup> </mrow> </semantics></math> is better, and it yields <span class="html-italic">τ<sub>a</sub></span> ≅ 150 μs.</p>
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<p>A <math display="inline"><semantics> <mrow> <mi>l</mi> <mi>o</mi> <mi>g</mi> <msup> <mrow> <mi>U</mi> </mrow> <mrow> <mi>*</mi> </mrow> </msup> </mrow> </semantics></math> versus <math display="inline"><semantics> <mrow> <mi>l</mi> <mi>o</mi> <mi>g</mi> <msup> <mrow> <mi>t</mi> </mrow> <mrow> <mi>*</mi> </mrow> </msup> </mrow> </semantics></math> plot from the tail region of <a href="#metals-15-00131-f008" class="html-fig">Figure 8</a>.</p>
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