Pub Date : 2024-09-07DOI: 10.1016/j.scriptamat.2024.116341
This study focuses on the impact of off-eutectic microstructures on mechanical properties in ternary Mo-Si-Ti alloys, namely Ti-rich Mo-18Si-72Ti and Mo-16.5Si-72Ti, in relation to the well-researched eutectic, two-phase Mo-20Si-52.8Ti alloy. The microstructure of these alloys consists of a Ti-rich body-centered cubic solid solution (Ti,Mo,Si)ss and a hexagonal silicide phase (Ti,Mo)5Si3. Notably, the off-eutectic alloys exhibit remarkable compression ductility at 800 °C, distinguishing it from Mo-20Si-52.8Ti. The directionally solidified (DS) specimens of the Ti-rich alloys display higher strength compared to the arc-melted specimens. This enhanced strength is attributed to the multiple precipitation strengthening events present, despite the increase in the length scale of individual phases which further enhances the fracture toughness.
{"title":"Strategic alloy design and processing for improved mechanical response in the Mo-Si-Ti system","authors":"","doi":"10.1016/j.scriptamat.2024.116341","DOIUrl":"10.1016/j.scriptamat.2024.116341","url":null,"abstract":"<div><p>This study focuses on the impact of off-eutectic microstructures on mechanical properties in ternary Mo-Si-Ti alloys, namely Ti-rich Mo-18Si-72Ti and Mo-16.5Si-72Ti, in relation to the well-researched eutectic, two-phase Mo-20Si-52.8Ti alloy. The microstructure of these alloys consists of a Ti-rich body-centered cubic solid solution (Ti,Mo,Si)<sub>ss</sub> and a hexagonal silicide phase (Ti,Mo)<sub>5</sub>Si<sub>3</sub>. Notably, the off-eutectic alloys exhibit remarkable compression ductility at 800 °C, distinguishing it from Mo-20Si-52.8Ti. The directionally solidified (DS) specimens of the Ti-rich alloys display higher strength compared to the arc-melted specimens. This enhanced strength is attributed to the multiple precipitation strengthening events present, despite the increase in the length scale of individual phases which further enhances the fracture toughness.</p></div>","PeriodicalId":423,"journal":{"name":"Scripta Materialia","volume":null,"pages":null},"PeriodicalIF":5.3,"publicationDate":"2024-09-07","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"https://www.sciencedirect.com/science/article/pii/S1359646224003750/pdfft?md5=5d1f51aaf8c6309c97451ddec900dc4d&pid=1-s2.0-S1359646224003750-main.pdf","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"142150379","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":2,"RegionCategory":"材料科学","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"OA","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
Pub Date : 2024-09-06DOI: 10.1016/j.scriptamat.2024.116355
Glasses in the TeO2-ZnO-Bi2O3 system were prepared with up to 2.5 mol% of Yb2O3 using standard melting process and their crystallization process was investigated for the first time. No concentration quenching was observed. The thermal treatment leads to surface precipitation of crystals, the composition of which depends on the Yb2O3 content. The addition of Yb2O3 in the tellurite network promotes the precipitation of Bi2Te4O11 crystals at the expense of Zn2Te3O8 crystals. The growing of these crystals in the low Yb3+ concentrated glass during a thermal treatment increases the interaction between the Yb3+ ions leading to an enhancement of the Yb3+ emission properties which reach those of highly Yb3+ concentrated tellurite glass. Our study suggests that a thermal treatment can be a practical alternative to increase the emission efficiency of the glass prepared with 0.5 mol% of Yb2O3 to the level of the as-prepared glass doped with 2.5 mol% of Yb2O3.
{"title":"Emission efficiency at 1 µm from low Yb3+ concentrated tellurite glass-ceramics: Alternative materials for the future rare-earth metal shortage","authors":"","doi":"10.1016/j.scriptamat.2024.116355","DOIUrl":"10.1016/j.scriptamat.2024.116355","url":null,"abstract":"<div><p>Glasses in the TeO<sub>2</sub>-ZnO-Bi<sub>2</sub>O<sub>3</sub> system were prepared with up to 2.5 mol% of Yb<sub>2</sub>O<sub>3</sub> using standard melting process and their crystallization process was investigated for the first time. No concentration quenching was observed. The thermal treatment leads to surface precipitation of crystals, the composition of which depends on the Yb<sub>2</sub>O<sub>3</sub> content. The addition of Yb<sub>2</sub>O<sub>3</sub> in the tellurite network promotes the precipitation of Bi<sub>2</sub>Te<sub>4</sub>O<sub>11</sub> crystals at the expense of Zn<sub>2</sub>Te<sub>3</sub>O<sub>8</sub> crystals. The growing of these crystals in the low Yb<sup>3+</sup> concentrated glass during a thermal treatment increases the interaction between the Yb<sup>3+</sup> ions leading to an enhancement of the Yb<sup>3+</sup> emission properties which reach those of highly Yb<sup>3+</sup> concentrated tellurite glass. Our study suggests that a thermal treatment can be a practical alternative to increase the emission efficiency of the glass prepared with 0.5 mol% of Yb<sub>2</sub>O<sub>3</sub> to the level of the as-prepared glass doped with 2.5 mol% of Yb<sub>2</sub>O<sub>3</sub>.</p></div>","PeriodicalId":423,"journal":{"name":"Scripta Materialia","volume":null,"pages":null},"PeriodicalIF":5.3,"publicationDate":"2024-09-06","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"https://www.sciencedirect.com/science/article/pii/S1359646224003907/pdfft?md5=601ac6bf22034ae752a33dac522778ce&pid=1-s2.0-S1359646224003907-main.pdf","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"142150561","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":2,"RegionCategory":"材料科学","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"OA","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
Pub Date : 2024-09-05DOI: 10.1016/j.scriptamat.2024.116343
Interfacial behavior in composites significantly influences their properties. Ag-based composites reinforced with Ti3AlC2 (a MAX phase) are promising for electrical contacts. However, interdiffusion between the Ag matrix and Ti3AlC2 increases impurities in the Ag matrix, adversely affecting electrical resistance and raising operational temperatures. To address this, we developed a novel partial etching pretreatment that selectively etches Al atoms from the near-surface region of Ti3AlC2, creating a Ti3C2 surface layer. This innovative approach confines interdiffusion mainly within the Ti3C2 layer, preserving the Ag matrix's high electrical conductivity. Experimental results for Ag-based composites with 10 wt.% of Ti3AlC2, subjected to 0.5 h etching, show a significant 51 % reduction in electrical resistivity with only a 10 % decrease in mechanical properties compared to Ag/Ti3AlC2. These findings underscore the effectiveness of manipulating A-site elements in Ti3AlC2 to enhance the performance of Ag-based composites, offering valuable insights for advanced electrical material design.
{"title":"Achieving highly conductive Ag/Ti3AlC2 composite by inhibiting interdiffusion","authors":"","doi":"10.1016/j.scriptamat.2024.116343","DOIUrl":"10.1016/j.scriptamat.2024.116343","url":null,"abstract":"<div><p>Interfacial behavior in composites significantly influences their properties. Ag-based composites reinforced with Ti<sub>3</sub>AlC<sub>2</sub> (a MAX phase) are promising for electrical contacts. However, interdiffusion between the Ag matrix and Ti<sub>3</sub>AlC<sub>2</sub> increases impurities in the Ag matrix, adversely affecting electrical resistance and raising operational temperatures. To address this, we developed a novel partial etching pretreatment that selectively etches Al atoms from the near-surface region of Ti<sub>3</sub>AlC<sub>2</sub>, creating a Ti<sub>3</sub>C<sub>2</sub> surface layer. This innovative approach confines interdiffusion mainly within the Ti<sub>3</sub>C<sub>2</sub> layer, preserving the Ag matrix's high electrical conductivity. Experimental results for Ag-based composites with 10 wt.% of Ti<sub>3</sub>AlC<sub>2</sub>, subjected to 0.5 h etching, show a significant 51 % reduction in electrical resistivity with only a 10 % decrease in mechanical properties compared to Ag/Ti<sub>3</sub>AlC<sub>2</sub>. These findings underscore the effectiveness of manipulating A-site elements in Ti<sub>3</sub>AlC<sub>2</sub> to enhance the performance of Ag-based composites, offering valuable insights for advanced electrical material design.</p></div>","PeriodicalId":423,"journal":{"name":"Scripta Materialia","volume":null,"pages":null},"PeriodicalIF":5.3,"publicationDate":"2024-09-05","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"142150560","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":2,"RegionCategory":"材料科学","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
Pub Date : 2024-09-05DOI: 10.1016/j.scriptamat.2024.116350
Physical modeling and deep learning are known for their respective advantages in interpretability and computational efficiency. Nonetheless, efficiently predicting properties of metallic materials while maintaining interpretability presents a formidable challenge. This study proposes a novel solution by introducing dual-output deep learning model that simultaneously predicts stress-strain partitioning and mechanical properties through a two-component architecture. The initial component uses U-Net model trained on stress and strain partitioning generated from crystal plasticity (CP) simulations, thereby enhancing interpretability. Subsequently, this information is used to predict the properties in the second component. The prediction results demonstrate the validity of this approach, accurately predicting high stress at the martensite-martensite interface, high strain at the ferrite-martensite interface, and properties. In addition, the minimal computational cost significantly improves efficiency compared to conventional CP method. This innovative methodology represents a significant advancement, achieving harmonious balance between interpretability, computational accuracy, and efficiency in properties prediction of metallic materials.
{"title":"Harmonizing physical and deep learning modeling: A computationally efficient and interpretable approach for property prediction","authors":"","doi":"10.1016/j.scriptamat.2024.116350","DOIUrl":"10.1016/j.scriptamat.2024.116350","url":null,"abstract":"<div><p>Physical modeling and deep learning are known for their respective advantages in interpretability and computational efficiency. Nonetheless, efficiently predicting properties of metallic materials while maintaining interpretability presents a formidable challenge. This study proposes a novel solution by introducing dual-output deep learning model that simultaneously predicts stress-strain partitioning and mechanical properties through a two-component architecture. The initial component uses U-Net model trained on stress and strain partitioning generated from crystal plasticity (CP) simulations, thereby enhancing interpretability. Subsequently, this information is used to predict the properties in the second component. The prediction results demonstrate the validity of this approach, accurately predicting high stress at the martensite-martensite interface, high strain at the ferrite-martensite interface, and properties. In addition, the minimal computational cost significantly improves efficiency compared to conventional CP method. This innovative methodology represents a significant advancement, achieving harmonious balance between interpretability, computational accuracy, and efficiency in properties prediction of metallic materials.</p></div>","PeriodicalId":423,"journal":{"name":"Scripta Materialia","volume":null,"pages":null},"PeriodicalIF":5.3,"publicationDate":"2024-09-05","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"142150558","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":2,"RegionCategory":"材料科学","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
Pub Date : 2024-09-05DOI: 10.1016/j.scriptamat.2024.116354
The optical transmission, the wavelength and temperature dependence of the Verdet constant as well as the thermally induced depolarization in a Zn4B6O13 crystal were investigated. The analytical dependence of the Verdet constant on wavelength and temperature, which describes well the experimental data in the 240–1100 nm range, was obtained. The small coefficient of linear expansion and its isotropy significantly suppressed thermally induced depolarization associated with thermally induced linear birefringence caused by the photo-elastic effect, while the diamagnetic nature of the material ensured the absence of thermally induced depolarization associated with the temperature dependence of the Verdet constant. The results revealed that Zn4B6O13 is highly suitable for the wavelength range of 248–350 nm and can be used as a magneto-optical material for an optical isolator for high-average-power UV lasers.
{"title":"Near-zero thermal expansion diamagnetic as a magneto-optical material for Faraday isolators for high power laser radiation","authors":"","doi":"10.1016/j.scriptamat.2024.116354","DOIUrl":"10.1016/j.scriptamat.2024.116354","url":null,"abstract":"<div><p>The optical transmission, the wavelength and temperature dependence of the Verdet constant as well as the thermally induced depolarization in a Zn<sub>4</sub>B<sub>6</sub>O<sub>13</sub> crystal were investigated. The analytical dependence of the Verdet constant on wavelength and temperature, which describes well the experimental data in the 240–1100 nm range, was obtained. The small coefficient of linear expansion and its isotropy significantly suppressed thermally induced depolarization associated with thermally induced linear birefringence caused by the photo-elastic effect, while the diamagnetic nature of the material ensured the absence of thermally induced depolarization associated with the temperature dependence of the Verdet constant. The results revealed that Zn<sub>4</sub>B<sub>6</sub>O<sub>13</sub> is highly suitable for the wavelength range of 248–350 nm and can be used as a magneto-optical material for an optical isolator for high-average-power UV lasers.</p></div>","PeriodicalId":423,"journal":{"name":"Scripta Materialia","volume":null,"pages":null},"PeriodicalIF":5.3,"publicationDate":"2024-09-05","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"142150557","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":2,"RegionCategory":"材料科学","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
Pub Date : 2024-09-05DOI: 10.1016/j.scriptamat.2024.116344
The high cost of noble metal raw materials is a major limitation to the production of hydrogen from electrocatalytic water splitting. Nowadays, the poor activity and complex synthesis methods of non-noble electrocatalysts need to be urgently improved. Herein, we prepared the Fe-Si-B alloys with nanosheet structure on the surface by de-alloying process in KOH solution. Experimental results indicate that there are lots of B-doped Fe nanosheets on the surface due to the faster dissolution rate of Fe-Si phase in the alkaline solution. The small amounts of boron remaining and the oxidation of the Fe nanosheets could enhance the activity of the hydrogen evolution reaction (HER). The HER overpotential under 10 mA/cm2 is 214 mV. The coordination between elemental components and the de-alloying process not only increased the electrochemical surface area, but also enhanced electrocatalytic activity of iron atoms. This work provides a new idea for the design of Fe-based electrocatalysts.
{"title":"De-alloyed non-noble Fe-based alloy for hydrogen evolution reaction","authors":"","doi":"10.1016/j.scriptamat.2024.116344","DOIUrl":"10.1016/j.scriptamat.2024.116344","url":null,"abstract":"<div><p>The high cost of noble metal raw materials is a major limitation to the production of hydrogen from electrocatalytic water splitting. Nowadays, the poor activity and complex synthesis methods of non-noble electrocatalysts need to be urgently improved. Herein, we prepared the Fe-Si-B alloys with nanosheet structure on the surface by de-alloying process in KOH solution. Experimental results indicate that there are lots of B-doped Fe nanosheets on the surface due to the faster dissolution rate of Fe-Si phase in the alkaline solution. The small amounts of boron remaining and the oxidation of the Fe nanosheets could enhance the activity of the hydrogen evolution reaction (HER). The HER overpotential under 10 mA/cm<sup>2</sup> is 214 mV. The coordination between elemental components and the de-alloying process not only increased the electrochemical surface area, but also enhanced electrocatalytic activity of iron atoms. This work provides a new idea for the design of Fe-based electrocatalysts.</p></div>","PeriodicalId":423,"journal":{"name":"Scripta Materialia","volume":null,"pages":null},"PeriodicalIF":5.3,"publicationDate":"2024-09-05","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"142150559","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":2,"RegionCategory":"材料科学","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
Pub Date : 2024-09-04DOI: 10.1016/j.scriptamat.2024.116351
In this study, three-dimensional functionally graded NiTi bulk materials were fabricated using laser powder bed fusion (LPBF) by in-situ adding Ni powder into equiatomic NiTi powder. The gradient zone exhibited a Ni composition ranging from approximately 49.6 to 52.4 at.% over a distance of about 2.75 mm. The functionalities along the compositional gradient were examined through differential scanning calorimetry analysis and spherical indentation. This unique gradient resulted in location-specific functionalities, including superelasticity characterized by wide and narrow hysteresis loops, shape memory effect, and various phase transformation temperatures. The rapid cooling rate during fabrication led to the presence of excess Ni in the solid-solute state within NiTi. This unique solid-solute compositional gradient in NiTi resulted in varying lattice parameters, influencing the compatibility between martensite and austenite and allowing for tailored hysteresis. This discovery presents new avenues for designing multifunctional materials through in-situ additive manufacturing.
{"title":"Functionally graded nickel–titanium shape memory alloys produced by in-situ additive manufacturing","authors":"","doi":"10.1016/j.scriptamat.2024.116351","DOIUrl":"10.1016/j.scriptamat.2024.116351","url":null,"abstract":"<div><p>In this study, three-dimensional functionally graded NiTi bulk materials were fabricated using laser powder bed fusion (LPBF) by <em>in-situ</em> adding Ni powder into equiatomic NiTi powder. The gradient zone exhibited a Ni composition ranging from approximately 49.6 to 52.4 at.% over a distance of about 2.75 mm. The functionalities along the compositional gradient were examined through differential scanning calorimetry analysis and spherical indentation. This unique gradient resulted in location-specific functionalities, including superelasticity characterized by wide and narrow hysteresis loops, shape memory effect, and various phase transformation temperatures. The rapid cooling rate during fabrication led to the presence of excess Ni in the solid-solute state within NiTi. This unique solid-solute compositional gradient in NiTi resulted in varying lattice parameters, influencing the compatibility between martensite and austenite and allowing for tailored hysteresis. This discovery presents new avenues for designing multifunctional materials through <em>in-situ</em> additive manufacturing.</p></div>","PeriodicalId":423,"journal":{"name":"Scripta Materialia","volume":null,"pages":null},"PeriodicalIF":5.3,"publicationDate":"2024-09-04","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"https://www.sciencedirect.com/science/article/pii/S1359646224003865/pdfft?md5=263e7b32b56d6a13f21da0fa8a502c86&pid=1-s2.0-S1359646224003865-main.pdf","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"142137183","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":2,"RegionCategory":"材料科学","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"OA","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
Pub Date : 2024-09-04DOI: 10.1016/j.scriptamat.2024.116345
Kagome lattice, made of corner-sharing triangles, provides an excellent platform for hosting exotic topological quantum phases. Here, we report the observation of large anomalous Hall effect and topological Hall effect in the Kagome lattice material Yb0.90Mn6Ge3.25Ga0.39 single crystal. Compared to the antiferromagnetic pristine compound YbMn6Ge6, Yb0.90Mn6Ge3.25Ga0.39 has an easy plane ferromagnetic structure below 361 K and presents a spin-reorientation transition at 218 K. An intrinsic anomalous Hall conductivity with the value of 604.2 Ω-1·cm-1 is obtained in Yb0.90Mn6Ge3.25Ga0.39, which is the largest in RMn6X6 (X = Ge and Sn) family. Besides, a remarkable topological Hall signal is also observed near room temperature. The topological Hall resistivity of Yb0.90Mn6Ge3.25Ga0.39 is determined to be -1.86 μΩ·cm at 280 K under μ0H = 0.3 T. Our results indicate that Yb0.90Mn6Ge3.25Ga0.39 may be an excellent platform to study the relationship between the magnetic and electronic structure and to explore novel quantum phenomenon.
由分角三角形组成的 Kagome 晶格为容纳奇异的拓扑量子相提供了一个极好的平台。在这里,我们报告了在 Kagome 晶格材料 Yb0.90Mn6Ge3.25Ga0.39 单晶中观察到的大反常霍尔效应和拓扑霍尔效应。与反铁磁性原始化合物 YbMn6Ge6 相比,Yb0.90Mn6Ge3.25Ga0.39 在 361 K 以下具有简单的平面铁磁性结构,并在 218 K 时出现自旋取向转变。此外,在室温附近还观察到了显著的拓扑霍尔信号。我们的结果表明,Yb0.90Mn6Ge3.25Ga0.39 可能是研究磁结构与电子结构之间关系以及探索新量子现象的绝佳平台。
{"title":"Anomalous Hall effect and topological Hall effect in Kagome lattice material Yb0.90Mn6Ge3.25Ga0.39 single crystal","authors":"","doi":"10.1016/j.scriptamat.2024.116345","DOIUrl":"10.1016/j.scriptamat.2024.116345","url":null,"abstract":"<div><p>Kagome lattice, made of corner-sharing triangles, provides an excellent platform for hosting exotic topological quantum phases. Here, we report the observation of large anomalous Hall effect and topological Hall effect in the Kagome lattice material Yb<sub>0.90</sub>Mn<sub>6</sub>Ge<sub>3.25</sub>Ga<sub>0.39</sub> single crystal. Compared to the antiferromagnetic pristine compound YbMn<sub>6</sub>Ge<sub>6</sub>, Yb<sub>0.90</sub>Mn<sub>6</sub>Ge<sub>3.25</sub>Ga<sub>0.39</sub> has an easy plane ferromagnetic structure below 361 K and presents a spin-reorientation transition at 218 K. An intrinsic anomalous Hall conductivity with the value of 604.2 Ω<sup>-1</sup>·cm<sup>-1</sup> is obtained in Yb<sub>0.90</sub>Mn<sub>6</sub>Ge<sub>3.25</sub>Ga<sub>0.39</sub>, which is the largest in RMn<sub>6</sub>X<sub>6</sub> (X = Ge and Sn) family. Besides, a remarkable topological Hall signal is also observed near room temperature. The topological Hall resistivity of Yb<sub>0.90</sub>Mn<sub>6</sub>Ge<sub>3.25</sub>Ga<sub>0.39</sub> is determined to be -1.86 μΩ·cm at 280 K under <em>μ</em><sub>0</sub><em>H</em> = 0.3 T. Our results indicate that Yb<sub>0.90</sub>Mn<sub>6</sub>Ge<sub>3.25</sub>Ga<sub>0.39</sub> may be an excellent platform to study the relationship between the magnetic and electronic structure and to explore novel quantum phenomenon.</p></div>","PeriodicalId":423,"journal":{"name":"Scripta Materialia","volume":null,"pages":null},"PeriodicalIF":5.3,"publicationDate":"2024-09-04","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"142137182","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":2,"RegionCategory":"材料科学","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
Pub Date : 2024-09-03DOI: 10.1016/j.scriptamat.2024.116340
The phase evolution in the transition zone (TZ) of TiAl/Ti2AlNb dual alloy during laser-directed energy deposition (L-DED) process was investigated using in situ synchrotron radiation X-ray diffraction. The as-solidified microstructure of the TZ forms through the following phase transitions: Liquid→ Liquid + β/B2 →β/B2→ β/B2 + α2. Thermal cycles promote the β/B2 to α2 phase transition with the α2 phase precipitates from the (011) plane of the β/B2 matrix during this transition. The phase transition sequence of the TZ during the first thermal cycle is: β/B2 + α2 → β/B2 → β/B2 + α2. The second thermal cycle leads to a partial transformation of β/B2 phase to α2 phase. The TZ experiences no phase transition from the third thermal cycle. This study provides a comprehensive understanding of the phase formation mechanism in the TZ of L-DEDed TiAl/Ti2AlNb dual alloys.
{"title":"In situ synchrotron X-ray diffraction study: Phase evolution in transition zone of TiAl/Ti2AlNb dual alloy fabricated by laser-directed energy deposition","authors":"","doi":"10.1016/j.scriptamat.2024.116340","DOIUrl":"10.1016/j.scriptamat.2024.116340","url":null,"abstract":"<div><p>The phase evolution in the transition zone (TZ) of TiAl/Ti<sub>2</sub>AlNb dual alloy during laser-directed energy deposition (L-DED) process was investigated using in situ synchrotron radiation X-ray diffraction. The as-solidified microstructure of the TZ forms through the following phase transitions: Liquid→ Liquid + β/B2 →β/B2→ β/B2 + α<sub>2</sub>. Thermal cycles promote the β/B2 to α<sub>2</sub> phase transition with the α<sub>2</sub> phase precipitates from the (011) plane of the β/B2 matrix during this transition. The phase transition sequence of the TZ during the first thermal cycle is: β/B2 + α<sub>2</sub> → β/B2 → β/B2 + α<sub>2</sub>. The second thermal cycle leads to a partial transformation of β/B2 phase to α<sub>2</sub> phase. The TZ experiences no phase transition from the third thermal cycle. This study provides a comprehensive understanding of the phase formation mechanism in the TZ of L-DEDed TiAl/Ti<sub>2</sub>AlNb dual alloys.</p></div>","PeriodicalId":423,"journal":{"name":"Scripta Materialia","volume":null,"pages":null},"PeriodicalIF":5.3,"publicationDate":"2024-09-03","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"142129690","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":2,"RegionCategory":"材料科学","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
Pub Date : 2024-09-03DOI: 10.1016/j.scriptamat.2024.116349
Significant effects of electric currents on mass transport in liquid metals have been observed for long, but the origin of the corresponding driving forces remains unclear in the literature. Without current, two driving forces induce mass transport in liquid metals. (i) A chemical force, coming from concentration gradients. In that case, mass transport occurs by diffusion. (ii) A physical force, resulting from density gradients thermally and/or chemically induced. Here, mass transport occurs by thermal and/or solutal convection. Under electric currents, these driving forces are modified, either by electrostatic or magnetic forces, the corresponding mechanisms being referred to as electroconvection and magnetoconvection, respectively. However, these mechanisms cannot easily be distinguished from each other, leading to confusion in literature. Here, it has been shown that, in the liquid Sn-Zn system, the driving force induced by 500–1000 A/cm2 electric current densities is magnetic rather than electrostatic, the mechanism being therefore magnetoconvection.
{"title":"Mass transport driving forces under electric current in the liquid Sn-Zn system","authors":"","doi":"10.1016/j.scriptamat.2024.116349","DOIUrl":"10.1016/j.scriptamat.2024.116349","url":null,"abstract":"<div><p>Significant effects of electric currents on mass transport in liquid metals have been observed for long, but the origin of the corresponding driving forces remains unclear in the literature. Without current, two driving forces induce mass transport in liquid metals. (i) A chemical force, coming from concentration gradients. In that case, mass transport occurs by diffusion. (ii) A physical force, resulting from density gradients thermally and/or chemically induced. Here, mass transport occurs by thermal and/or solutal convection. Under electric currents, these driving forces are modified, either by electrostatic or magnetic forces, the corresponding mechanisms being referred to as electroconvection and magnetoconvection, respectively. However, these mechanisms cannot easily be distinguished from each other, leading to confusion in literature. Here, it has been shown that, in the liquid Sn-Zn system, the driving force induced by 500–1000 A/cm<sup>2</sup> electric current densities is magnetic rather than electrostatic, the mechanism being therefore magnetoconvection.</p></div>","PeriodicalId":423,"journal":{"name":"Scripta Materialia","volume":null,"pages":null},"PeriodicalIF":5.3,"publicationDate":"2024-09-03","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"https://www.sciencedirect.com/science/article/pii/S1359646224003841/pdfft?md5=2300451f648aed5b1d0eaffabc8241e5&pid=1-s2.0-S1359646224003841-main.pdf","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"142129691","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":2,"RegionCategory":"材料科学","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"OA","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}