Pub Date : 2024-09-18DOI: 10.1007/s11661-024-07563-w
Sindo Kou
Grain refining is of practical interest in welding, casting, and additive manufacturing. Despite extensive studies, it is still not very clear why grain refining can decrease the susceptibility to cracking during solidification and why over grain refining can increase it. To help understand why, the present study included the continuity of the interdendritic liquid and solute poisoning into consideration. The present study also attempted to estimate the decrease in the cracking susceptibility caused by grain refining. To do this, a simple index for the cracking susceptibility was modified by the extent of grain refining. The validity of the estimation was checked against cracking susceptibility tests in welding and casting.
{"title":"Grain Refining and Cracking During Solidification","authors":"Sindo Kou","doi":"10.1007/s11661-024-07563-w","DOIUrl":"https://doi.org/10.1007/s11661-024-07563-w","url":null,"abstract":"<p>Grain refining is of practical interest in welding, casting, and additive manufacturing. Despite extensive studies, it is still not very clear why grain refining can decrease the susceptibility to cracking during solidification and why over grain refining can increase it. To help understand why, the present study included the continuity of the interdendritic liquid and solute poisoning into consideration. The present study also attempted to estimate the decrease in the cracking susceptibility caused by grain refining. To do this, a simple index for the cracking susceptibility was modified by the extent of grain refining. The validity of the estimation was checked against cracking susceptibility tests in welding and casting.</p>","PeriodicalId":18504,"journal":{"name":"Metallurgical and Materials Transactions A","volume":"28 1","pages":""},"PeriodicalIF":0.0,"publicationDate":"2024-09-18","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"142267162","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":0,"RegionCategory":"","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
Pub Date : 2024-09-16DOI: 10.1007/s11661-024-07590-7
Mohammad Javad Sohrabi, Hamed Mirzadeh, Saeed Sadeghpour, Reza Mahmudi, Alireza Kalhor, Kinga Rodak, Hyoung Seop Kim
Microstructural evolutions and cryogenic mechanical properties of AISI 904L superaustenitic stainless steel were studied for the first time and compared with those of metastable AISI 304L and 316L austenitic stainless steels. The temperature-dependencies of these properties were critically discussed and correlated to the microstructures, focusing on the solid solution strengthening, transformation-induced plasticity (TRIP), and twinning-induced plasticity (TWIP) effects. The 904L alloy showed an extraordinary cryogenic strength-ductility synergy with excellent work-hardening behavior.
{"title":"Remarkable Cryogenic Strength and Ductility of AISI 904L Superaustenitic Stainless Steel: A Comparative Study","authors":"Mohammad Javad Sohrabi, Hamed Mirzadeh, Saeed Sadeghpour, Reza Mahmudi, Alireza Kalhor, Kinga Rodak, Hyoung Seop Kim","doi":"10.1007/s11661-024-07590-7","DOIUrl":"https://doi.org/10.1007/s11661-024-07590-7","url":null,"abstract":"<p>Microstructural evolutions and cryogenic mechanical properties of AISI 904L superaustenitic stainless steel were studied for the first time and compared with those of metastable AISI 304L and 316L austenitic stainless steels. The temperature-dependencies of these properties were critically discussed and correlated to the microstructures, focusing on the solid solution strengthening, transformation-induced plasticity (TRIP), and twinning-induced plasticity (TWIP) effects. The 904L alloy showed an extraordinary cryogenic strength-ductility synergy with excellent work-hardening behavior.</p>","PeriodicalId":18504,"journal":{"name":"Metallurgical and Materials Transactions A","volume":"20 1","pages":""},"PeriodicalIF":0.0,"publicationDate":"2024-09-16","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"142267188","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":0,"RegionCategory":"","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
Pub Date : 2024-09-16DOI: 10.1007/s11661-024-07580-9
S. Sun, C. M. Gourlay
The microstructure of electronic solder joints is generated by the solidification of a small volume of bulk undercooled liquid. Here, we study β-Sn dendrite growth in Sn–3Ag–0.5Cu in the specific geometry and nucleation conditions of ball grid array (BGA) solder joints by combining electron backscatter diffraction and imaging of microstructures. It is shown that, while (langle 110rangle) is the preferred dendrite growth direction, out-of-plane branching and growth with (langle 11Wrangle) directions are important for allowing dendrites to fan out into the spheroidal volume of BGA joints due to the low symmetry of β-Sn. We find that the crystallographic orientation of β-Sn at the nucleation point plays a strong role in subsequent dendrite growth. In single-grain joints, dendrites are often unfavorably oriented for growth, resulting in different types of zig-zag dendrite growth. In cyclic-twinned joints, it is shown how competitive out-of-plane trunk growth between three dendrite orientations produces {101} boundaries and the characteristic beachball microstructure.
{"title":"Dendrite Growth in Single-Grain and Cyclic-Twinned Sn–3Ag–0.5Cu Solder Joints","authors":"S. Sun, C. M. Gourlay","doi":"10.1007/s11661-024-07580-9","DOIUrl":"https://doi.org/10.1007/s11661-024-07580-9","url":null,"abstract":"<p>The microstructure of electronic solder joints is generated by the solidification of a small volume of bulk undercooled liquid. Here, we study <i>β</i>-Sn dendrite growth in Sn–3Ag–0.5Cu in the specific geometry and nucleation conditions of ball grid array (BGA) solder joints by combining electron backscatter diffraction and imaging of microstructures. It is shown that, while <span>(langle 110rangle)</span> is the preferred dendrite growth direction, out-of-plane branching and growth with <span>(langle 11Wrangle)</span> directions are important for allowing dendrites to fan out into the spheroidal volume of BGA joints due to the low symmetry of <i>β</i>-Sn. We find that the crystallographic orientation of <i>β</i>-Sn at the nucleation point plays a strong role in subsequent dendrite growth. In single-grain joints, dendrites are often unfavorably oriented for growth, resulting in different types of zig-zag dendrite growth. In cyclic-twinned joints, it is shown how competitive out-of-plane trunk growth between three dendrite orientations produces {101} boundaries and the characteristic beachball microstructure.</p>","PeriodicalId":18504,"journal":{"name":"Metallurgical and Materials Transactions A","volume":"98 1","pages":""},"PeriodicalIF":0.0,"publicationDate":"2024-09-16","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"142267185","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":0,"RegionCategory":"","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
Pub Date : 2024-09-13DOI: 10.1007/s11661-024-07583-6
Michał Falkowski, Jakub Kaczkowski, Grażyna Chełkowska, Andrzej Kowalczyk
We investigated the structural, elastic, vibrational, and electronic properties of the Nb5Si2B compound combining density functional theory (DFT) calculations and experimental methods. We compared our results with the parent compound Nb5Si3 with two non-equivalent Si sites namely Si(4a) and Si(8h). The analysis of elastic constants and phonon spectra indicate that Nb5Si2B is respectively mechanically and dynamically stable. Based on the phonon calculation we evaluate the theoretical constant volume lattice specific heat (CV) for different site occupancies and compare it with experimental specific heat (Cp) measurements. We found an excellent agreement between theoretical and experimental results for Nb5Si2B with the B at the Si(8h) site, which agrees with the calculated formation energy. In addition, we also performed DFT calculations aimed at showing and comparing the total DOS near the Fermi level (EF) for Nb5Si3 and Nb5Si2B. The XPS valence band (VB) of the Nb5Si2B is largely dominated by two characteristic peaks at − 8.7 and − 1.7 eV, respectively. Based on DFT calculations, it follows that the main sharp peak at − 1.7 eV comes as a contribution from Nb 4d states, while the smaller and broader one located at − 8.7 eV results mainly from Si 3s states weakly hybridized with Nb 4d states. In this connection, the majority contribution in the binding energy range from − 12 eV to the EF comes from Nb 4d states, while the contribution from Si and B atoms is very small in this region. The core levels of Nb 3d, Si 2s, 2p, and B 1s were also identified using the XPS technique.
我们结合密度泛函理论(DFT)计算和实验方法,研究了 Nb5Si2B 化合物的结构、弹性、振动和电子特性。我们将研究结果与具有两个非等效 Si 位点(即 Si(4a)和 Si(8h))的母体化合物 Nb5Si3 进行了比较。弹性常数和声子频谱分析表明,Nb5Si2B 分别具有机械稳定性和动力学稳定性。在声子计算的基础上,我们评估了不同位点占有率下的理论恒定体积晶格比热(CV),并将其与实验比热(Cp)测量值进行了比较。我们发现,对于 B 位于 Si(8h)位的 Nb5Si2B,理论和实验结果非常一致,这与计算得出的形成能相吻合。此外,我们还进行了 DFT 计算,旨在显示和比较 Nb5Si3 和 Nb5Si2B 费米水平 (EF) 附近的总 DOS。Nb5Si2B 的 XPS 价带 (VB) 主要由分别位于 - 8.7 和 - 1.7 eV 的两个特征峰所主导。根据 DFT 计算,- 1.7 eV 处的尖锐主峰来自 Nb 4d 态,而位于 - 8.7 eV 处的较小较宽的主峰主要来自与 Nb 4d 态弱杂化的 Si 3s 态。因此,在- 12 eV到EF的结合能范围内,大部分贡献来自铌4d态,而来自硅和B原子的贡献在这一区域非常小。利用 XPS 技术还确定了 Nb 3d、Si 2s、2p 和 B 1s 的核心水平。
{"title":"The Effect of Silicon Substitution by Boron for the α-Nb5Si3: INSIGHTS into the Constitutive Properties of Nb5Si2B Through Theory and Experimental Approach","authors":"Michał Falkowski, Jakub Kaczkowski, Grażyna Chełkowska, Andrzej Kowalczyk","doi":"10.1007/s11661-024-07583-6","DOIUrl":"https://doi.org/10.1007/s11661-024-07583-6","url":null,"abstract":"<p>We investigated the structural, elastic, vibrational, and electronic properties of the Nb<sub>5</sub>Si<sub>2</sub>B compound combining density functional theory (DFT) calculations and experimental methods. We compared our results with the parent compound Nb<sub>5</sub>Si<sub>3</sub> with two non-equivalent Si sites namely Si(4a) and Si(8h). The analysis of elastic constants and phonon spectra indicate that Nb<sub>5</sub>Si<sub>2</sub>B is respectively mechanically and dynamically stable. Based on the phonon calculation we evaluate the theoretical constant volume lattice specific heat (<i>C</i><sub>V</sub>) for different site occupancies and compare it with experimental specific heat (<i>C</i><sub>p</sub>) measurements. We found an excellent agreement between theoretical and experimental results for Nb<sub>5</sub>Si<sub>2</sub>B with the B at the Si(8h) site, which agrees with the calculated formation energy. In addition, we also performed DFT calculations aimed at showing and comparing the total DOS near the Fermi level (<i>E</i><sub>F</sub>) for Nb<sub>5</sub>Si<sub>3</sub> and Nb<sub>5</sub>Si<sub>2</sub>B. The XPS valence band (VB) of the Nb<sub>5</sub>Si<sub>2</sub>B is largely dominated by two characteristic peaks at − 8.7 and − 1.7 eV, respectively. Based on DFT calculations, it follows that the main sharp peak at − 1.7 eV comes as a contribution from Nb 4d states, while the smaller and broader one located at − 8.7 eV results mainly from Si 3s states weakly hybridized with Nb 4d states. In this connection, the majority contribution in the binding energy range from − 12 eV to the <i>E</i><sub>F</sub> comes from Nb 4d states, while the contribution from Si and B atoms is very small in this region. The core levels of Nb 3d, Si 2s, 2p, and B 1s were also identified using the XPS technique.</p>","PeriodicalId":18504,"journal":{"name":"Metallurgical and Materials Transactions A","volume":"567 1","pages":""},"PeriodicalIF":0.0,"publicationDate":"2024-09-13","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"142267190","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":0,"RegionCategory":"","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
Pub Date : 2024-09-13DOI: 10.1007/s11661-024-07585-4
Milena Kowalska, Paweł Czaja, Łukasz Rogal, Maciej J. Szczerba
The study brings original data on the effect of linear velocity during melt-spinning process on magneto-mechanical properties of Heusler Ni-Mn-Ga-based melt-spun ribbons. The research revealed that different linear velocity of the copper wheel had a significant impact on the ribbon's geometry resulting in distinct changes in magneto-mechanical properties. X-ray diffraction measurements were used to examine the phase composition, confirming the presence of L21 austenite phase. To assess the mechanical properties of the Ni-Mn-Ga-based melt-spun ribbons, cyclic bending experiments were conducted at a strain rate of 0.1 mm/s. Additionally, experiments involving magnetic field-induced bending were carried out in an external magnetic field ranging from 0 to 0.28 T. Finally, it was observed that there was a proportional relationship between the linear velocity of the copper wheel and magnetic field-induced ribbons deflection. Conversely, the dependence between linear velocity and mechanical bending load was found to be inversely proportional. Electron backscattered diffraction measurements revealed that melt-spun ribbons produced at high linear velocity of 18.5 m/s exhibited fine-grained microstructure in contrast to low linear velocity of 3 m/s. Based on these results it seems feasible to optimize the functional properties of the studied ribbons by varying the linear velocity of the melt-spinning process.
{"title":"Effect of Linear Velocity on Magneto-mechanical Properties of Ni-Mn-Ga-Based Melt-Spun Ribbons","authors":"Milena Kowalska, Paweł Czaja, Łukasz Rogal, Maciej J. Szczerba","doi":"10.1007/s11661-024-07585-4","DOIUrl":"https://doi.org/10.1007/s11661-024-07585-4","url":null,"abstract":"<p>The study brings original data on the effect of linear velocity during melt-spinning process on magneto-mechanical properties of Heusler Ni-Mn-Ga-based melt-spun ribbons. The research revealed that different linear velocity of the copper wheel had a significant impact on the ribbon's geometry resulting in distinct changes in magneto-mechanical properties. X-ray diffraction measurements were used to examine the phase composition, confirming the presence of L2<sub>1</sub> austenite phase. To assess the mechanical properties of the Ni-Mn-Ga-based melt-spun ribbons, cyclic bending experiments were conducted at a strain rate of 0.1 mm/s. Additionally, experiments involving magnetic field-induced bending were carried out in an external magnetic field ranging from 0 to 0.28 T. Finally, it was observed that there was a proportional relationship between the linear velocity of the copper wheel and magnetic field-induced ribbons deflection. Conversely, the dependence between linear velocity and mechanical bending load was found to be inversely proportional. Electron backscattered diffraction measurements revealed that melt-spun ribbons produced at high linear velocity of 18.5 m/s exhibited fine-grained microstructure in contrast to low linear velocity of 3 m/s. Based on these results it seems feasible to optimize the functional properties of the studied ribbons by varying the linear velocity of the melt-spinning process.</p>","PeriodicalId":18504,"journal":{"name":"Metallurgical and Materials Transactions A","volume":"21 1","pages":""},"PeriodicalIF":0.0,"publicationDate":"2024-09-13","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"142267191","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":0,"RegionCategory":"","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
Pub Date : 2024-09-13DOI: 10.1007/s11661-024-07579-2
Huamao Rao, Andrew Mullis, Robert Cochrane
The effect of rapid solidification upon hypereutectic Sn–Ag solder alloy has been investigated using a 6.5 m drop tube. Powder sizes ranging from > 850 to < 38 μm were produced, with equivalent cooling rates of 250 to 14,800 K s−1 for 850 and 38 μm droplets, respectively. At all cooling rates investigated, dendritic β-Sn was observed as the primary solidification phase, not proeutectic Ag3Sn as predicted by the phase diagram. The volume fraction of interdendritic eutectic was observed to decrease with increasing cooling rate, with the Ag concentration in the residual interdendritic liquid estimated at 12.5–15 wt pct Ag, far in excess of the eutectic concentration of 3.8 wt pct. Much of the Ag3Sn observed within the eutectic had a blocky, divorced eutectic appearance. A model is proposed which can explain these observations in terms of sluggish nucleation of the Ag3Sn intermetallic, coupled with a metastable phase diagram that permits significant supersaturation of Ag at modest undercooling.
{"title":"Eutectic Solidification Morphologies in Rapidly Solidified Hypereutectic Sn–Ag Solder Alloy","authors":"Huamao Rao, Andrew Mullis, Robert Cochrane","doi":"10.1007/s11661-024-07579-2","DOIUrl":"https://doi.org/10.1007/s11661-024-07579-2","url":null,"abstract":"<p>The effect of rapid solidification upon hypereutectic Sn–Ag solder alloy has been investigated using a 6.5 m drop tube. Powder sizes ranging from > 850 to < 38 <i>μ</i>m were produced, with equivalent cooling rates of 250 to 14,800 K s<sup>−1</sup> for 850 and 38 <i>μ</i>m droplets, respectively. At all cooling rates investigated, dendritic <i>β</i>-Sn was observed as the primary solidification phase, not proeutectic Ag<sub>3</sub>Sn as predicted by the phase diagram. The volume fraction of interdendritic eutectic was observed to decrease with increasing cooling rate, with the Ag concentration in the residual interdendritic liquid estimated at 12.5–15 wt pct Ag, far in excess of the eutectic concentration of 3.8 wt pct. Much of the Ag<sub>3</sub>Sn observed within the eutectic had a blocky, divorced eutectic appearance. A model is proposed which can explain these observations in terms of sluggish nucleation of the Ag<sub>3</sub>Sn intermetallic, coupled with a metastable phase diagram that permits significant supersaturation of Ag at modest undercooling.</p>","PeriodicalId":18504,"journal":{"name":"Metallurgical and Materials Transactions A","volume":"16 1","pages":""},"PeriodicalIF":0.0,"publicationDate":"2024-09-13","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"142267187","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":0,"RegionCategory":"","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
Selective laser-melted 316L stainless steel (SLM 316L SS) holds significant potential for application in the energy and chemical sectors owing to its commendable mechanical properties and corrosion resistance. However, the intricate process of microstructure evolution in SLM 316L SS at intermediate temperatures, encompassing the feasible range of service temperatures, needs to be more adequately comprehended. This research endeavors to elucidate the grain size and distribution alterations between 750 °C and 850 °C. Abnormal grain growth before recrystallization and re-refinement phenomena were observed, which deviated from conventional expectations. The texture was found to play a crucial role in former, while recovery-induced dislocation rearrangement and recrystallization nuclei formation contributed to the latter process. These findings provide new insights into the thermodynamic behavior of SLM 316L SS at medium to high temperatures.
Graphical Abstract
选择性激光熔融 316L 不锈钢(SLM 316L SS)具有良好的机械性能和耐腐蚀性,因此在能源和化工领域有着巨大的应用潜力。然而,SLM 316L 不锈钢在中间温度(包括可行的使用温度范围)下微观结构演变的复杂过程需要得到更充分的理解。本研究致力于阐明 750 °C 至 850 °C 之间晶粒大小和分布的变化。在再结晶和再细化现象之前观察到了异常的晶粒生长,这与传统的预期不同。发现纹理在前者中发挥了关键作用,而复原诱导的位错重排和再结晶核的形成则促成了后者。这些发现为 SLM 316L SS 在中高温下的热力学行为提供了新的见解。
{"title":"Recovery-Assisted Abnormal Grain Evolution of Selective Laser-Melted 316L Stainless Steel at Intermediate Temperatures","authors":"Yushi Xiao, Chao Wang, Yashan Zhang, Xinyi Liu, Chuntao Qin, Zhijun Wang, Xin Lin, Jincheng Wang, Lilin Wang, Feng He","doi":"10.1007/s11661-024-07578-3","DOIUrl":"https://doi.org/10.1007/s11661-024-07578-3","url":null,"abstract":"<p>Selective laser-melted 316L stainless steel (SLM 316L SS) holds significant potential for application in the energy and chemical sectors owing to its commendable mechanical properties and corrosion resistance. However, the intricate process of microstructure evolution in SLM 316L SS at intermediate temperatures, encompassing the feasible range of service temperatures, needs to be more adequately comprehended. This research endeavors to elucidate the grain size and distribution alterations between 750 °C and 850 °C. Abnormal grain growth before recrystallization and re-refinement phenomena were observed, which deviated from conventional expectations. The texture was found to play a crucial role in former, while recovery-induced dislocation rearrangement and recrystallization nuclei formation contributed to the latter process. These findings provide new insights into the thermodynamic behavior of SLM 316L SS at medium to high temperatures.</p><h3 data-test=\"abstract-sub-heading\">Graphical Abstract</h3>","PeriodicalId":18504,"journal":{"name":"Metallurgical and Materials Transactions A","volume":"10 1","pages":""},"PeriodicalIF":0.0,"publicationDate":"2024-09-12","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"142223426","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":0,"RegionCategory":"","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
Pub Date : 2024-09-12DOI: 10.1007/s11661-024-07581-8
X. Wang, J. Y. Wang, R. H. Xiao, W. Zhai, B. Wei
The introduction of one-dimensional (1D), two-dimensional (2D), and three-dimensional (3D) ultrasounds into solidifying FeCoNiCuAl high-entropy alloy was efficiently optimized, which realized the maximum input of acoustic energy and the effective adjustment of the energy proportion between stable and transient cavitation effects. In addition to the ordinary advantage of grain refinement, the superiority of power ultrasound in modulating such Cu-containing high-entropy alloys with dendritic structures mainly lay in the significant regulation of phase volume fraction and the elimination of severe Cu element microsegregation. As the main energy transmission form under 1D ultrasound, stable cavitation slightly increased the nucleation rate of α and γ1 phases, which jointly contributed to suppressing the Cu solute enrichment from 41.6 to 36 at pct through the acoustic streaming during the subsequent growth of γ1 phase. When 2D and 3D ultrasounds were applied, the intensive transient cavitation dominated the solidification process. The induced local high undercooling resulted in the competitive nucleation and growth between α and γ1 phases, leading to the more than one order of magnitude reduction in their grain sizes and the significant rise of γ1 phase volume fraction from 13 up to 50 pct. Meanwhile, it strikingly reduced the final Cu content difference between these two phases from over 30 to around 3.8 at pct by decreasing the Cu composition in competitively formed γ1 nuclei. The above microstructure modification brought in excellent compressive property for 3D ultrasonically solidified alloy, whose strength and ductility were simultaneously enhanced by 27 and 24 pct.
{"title":"Modulating Phase Constitution and Copper Microsegregation for FeCoNiCuAl High-Entropy Alloy by Optimized Ultrasonic Solidification","authors":"X. Wang, J. Y. Wang, R. H. Xiao, W. Zhai, B. Wei","doi":"10.1007/s11661-024-07581-8","DOIUrl":"https://doi.org/10.1007/s11661-024-07581-8","url":null,"abstract":"<p>The introduction of one-dimensional (1D), two-dimensional (2D), and three-dimensional (3D) ultrasounds into solidifying FeCoNiCuAl high-entropy alloy was efficiently optimized, which realized the maximum input of acoustic energy and the effective adjustment of the energy proportion between stable and transient cavitation effects. In addition to the ordinary advantage of grain refinement, the superiority of power ultrasound in modulating such Cu-containing high-entropy alloys with dendritic structures mainly lay in the significant regulation of phase volume fraction and the elimination of severe Cu element microsegregation. As the main energy transmission form under 1D ultrasound, stable cavitation slightly increased the nucleation rate of <i>α</i> and <i>γ</i><sub>1</sub> phases, which jointly contributed to suppressing the Cu solute enrichment from 41.6 to 36 at pct through the acoustic streaming during the subsequent growth of <i>γ</i><sub>1</sub> phase. When 2D and 3D ultrasounds were applied, the intensive transient cavitation dominated the solidification process. The induced local high undercooling resulted in the competitive nucleation and growth between <i>α</i> and <i>γ</i><sub>1</sub> phases, leading to the more than one order of magnitude reduction in their grain sizes and the significant rise of <i>γ</i><sub>1</sub> phase volume fraction from 13 up to 50 pct. Meanwhile, it strikingly reduced the final Cu content difference between these two phases from over 30 to around 3.8 at pct by decreasing the Cu composition in competitively formed <i>γ</i><sub>1</sub> nuclei. The above microstructure modification brought in excellent compressive property for 3D ultrasonically solidified alloy, whose strength and ductility were simultaneously enhanced by 27 and 24 pct.</p>","PeriodicalId":18504,"journal":{"name":"Metallurgical and Materials Transactions A","volume":"267 1","pages":""},"PeriodicalIF":0.0,"publicationDate":"2024-09-12","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"142177012","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":0,"RegionCategory":"","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
Pub Date : 2024-09-12DOI: 10.1007/s11661-024-07569-4
Joshua Kumpati, Manon Bonvalet Rolland, Sk. Md. Hasan, Katherine S. Shanks, Peter Hedström, Annika Borgenstam
Given the critical role that metastable retained austenite (RA) plays in advanced high-strength steel (AHSS), there is significant interest in obtaining a comprehensive understanding of its stability, to achieve excellent mechanical properties. Despite considerable attention and numerous studies, the significance of individual contributions of various microstructural factors (size, crystallographic orientation, surrounding phases, etc.) on the stability of RA remain unclear, partly due to the difficulty of isolating the direct effects of these factors. In this study, we examined the influence of microstructural factors while minimizing the effect of chemical composition on the mechanical stability of RA. We accomplished this by comparing the austenite (γ) stability in two distinct microstructures: a two-phase RA/martensite microstructure and a one-phase γ microstructure, both with nearly identical γ compositions. We employed in situ high-energy X-ray diffraction during uniaxial tensile testing conducted at both room temperature and 100 °C, facilitating the continuous monitoring of microstructural changes during the deformation process. By establishing a direct correlation between the macroscopic tensile load, phase load partitioning, and the γ/RA transformation, we aimed to understand the significance of the microstructural factors on the mechanical stability of the RA. The results indicate that very fine RA size and the surrounding hard martensitic matrix (aside from contributing to load partitioning) contribute less significantly to RA stability during deformation than expected. The findings of this study emphasize the critical and distinct influence of microstructure on γ/RA stability.
鉴于可转移残余奥氏体(RA)在先进高强度钢(AHSS)中的关键作用,人们对全面了解其稳定性以获得优异的机械性能产生了浓厚的兴趣。尽管受到了广泛关注并进行了大量研究,但各种微观结构因素(尺寸、结晶取向、周围相等)对 RA 稳定性的单独贡献意义仍不明确,部分原因是难以分离这些因素的直接影响。在本研究中,我们研究了微观结构因素的影响,同时尽量减少化学成分对 RA 机械稳定性的影响。为此,我们比较了两种不同微结构中奥氏体(γ)的稳定性:一种是两相 RA/马氏体微结构,另一种是单相 γ 微结构,两者的 γ 成分几乎完全相同。我们在室温和 100 °C 下进行的单轴拉伸测试中采用了原位高能 X 射线衍射技术,从而便于持续监测变形过程中的微观结构变化。通过建立宏观拉伸载荷、相载荷分配和 γ/RA 转变之间的直接相关性,我们旨在了解微观结构因素对 RA 机械稳定性的影响。结果表明,极细的 RA 尺寸和周围的硬质马氏体基体(除了对载荷分区有影响外)对 RA 在变形过程中的稳定性的影响比预期的要小。该研究结果强调了微观结构对γ/RA稳定性的关键和独特影响。
{"title":"Deconstructing the Retained Austenite Stability: In Situ Observations on the Austenite Stability in One- and Two-Phase Bulk Microstructures During Uniaxial Tensile Tests","authors":"Joshua Kumpati, Manon Bonvalet Rolland, Sk. Md. Hasan, Katherine S. Shanks, Peter Hedström, Annika Borgenstam","doi":"10.1007/s11661-024-07569-4","DOIUrl":"https://doi.org/10.1007/s11661-024-07569-4","url":null,"abstract":"<p>Given the critical role that metastable retained austenite (RA) plays in advanced high-strength steel (AHSS), there is significant interest in obtaining a comprehensive understanding of its stability, to achieve excellent mechanical properties. Despite considerable attention and numerous studies, the significance of individual contributions of various microstructural factors (size, crystallographic orientation, surrounding phases, <i>etc</i>.) on the stability of RA remain unclear, partly due to the difficulty of isolating the direct effects of these factors. In this study, we examined the influence of microstructural factors while minimizing the effect of chemical composition on the mechanical stability of RA. We accomplished this by comparing the austenite (γ) stability in two distinct microstructures: a two-phase RA/martensite microstructure and a one-phase γ microstructure, both with nearly identical γ compositions. We employed <i>in situ</i> high-energy X-ray diffraction during uniaxial tensile testing conducted at both room temperature and 100 °C, facilitating the continuous monitoring of microstructural changes during the deformation process. By establishing a direct correlation between the macroscopic tensile load, phase load partitioning, and the γ/RA transformation, we aimed to understand the significance of the microstructural factors on the mechanical stability of the RA. The results indicate that very fine RA size and the surrounding hard martensitic matrix (aside from contributing to load partitioning) contribute less significantly to RA stability during deformation than expected. The findings of this study emphasize the critical and distinct influence of microstructure on γ/RA stability.</p>","PeriodicalId":18504,"journal":{"name":"Metallurgical and Materials Transactions A","volume":"107 1","pages":""},"PeriodicalIF":0.0,"publicationDate":"2024-09-12","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"142177011","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":0,"RegionCategory":"","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
Pub Date : 2024-09-11DOI: 10.1007/s11661-024-07571-w
Niraj Kumar, Prakash Kumar, Ravi Shanker Vidyarthy, Chandan Pandey
For this study, the researchers aimed to dissimilar weld the Nickel-based superalloy Inconel 718 (IN 718) with austenitic stainless steel 304L (ASS 304L) using the gas tungsten arc welding (GTAW) technique and Nickel-based filler IN 82 (ERNiCr-3). In order to examine the weld microstructures, we utilized optical microscopy (OM) and field emission scanning electron microscopy (FESEM) with energy-dispersive spectroscopy (EDS) to identify any segregation present in various weld zones. Through optical and FESEM analyses, it was revealed that the base metals (BM) exhibit an austenitic character. The IN 718 BM matrix contains dispersed γ′ and γ″ strengthening precipitates within the Nickel matrix. On the other hand, the ASS 304L BM displayed a unique austenitic microstructure characterized by twins features. The weld metal exhibited solidification grain boundaries (SGBs), migrated grain boundaries (MGBs), and distinct dendritic microstructures that had an impact on the properties of the weld. Through extensive analysis and mapping of the IN 82 weld zone, it was discovered that interdendritic regions contain carbides of Nb, Cr, and Ti. In addition, there were Unmixed zone (UZ) areas between the IN 82 filler and the base materials on both sides of the weld zone, appearing as islands and beaches. The texture of the different weld zones was evaluated using electron backscattered diffraction (EBSD) analysis. Additionally, the presence of a notable level of strain within the weld metal grains was observed through Kernel average misorientation (KAM) micrographs. Fractures were observed in the IN 82 weld zone, indicating that it is the weakest area in the IN 718/ASS 304L dissimilar weld at room temperature, according to the outputs of the tensile tests. The micro-hardness profile showed substantial hardness values in the weld zone, which can be attributed to the appearance of a diverse microstructure and additional precipitates. At room temperature, the recorded average tensile strength of the dissimilar weld joint was 626 MPa. In addition, experiments were carried out at high temperatures of 550 °C, 600 °C, and 650 °C to measure the tensile strength. In the high-temperature tensile tests, it was observed that the IN 82 weld zone exhibited higher tensile strength compared to the ASS 304L BM. Interestingly, the high temperatures tensile specimens failed in the 304L BM. The Charpy impact toughness test was performed with notches at ASS 304L HAZ, IN 718 HAZ, and the weld center. Using the deep hole drilling (DHD) technique, we were able to quantify residual stress and identify the location of the highest tensile residual stress, which was found to be 3 mm from the weld surface.
在这项研究中,研究人员采用气体钨极氩弧焊(GTAW)技术和镍基填料 IN 82 (ERNiCr-3) 对镍基超级合金 Inconel 718 (IN 718) 和奥氏体不锈钢 304L (ASS 304L) 进行了异种焊接。为了检查焊缝的微观结构,我们使用了光学显微镜(OM)和场发射扫描电子显微镜(FESEM)以及能量色散光谱仪(EDS),以确定各焊接区是否存在偏析。通过光学和场发射扫描电子显微镜分析发现,基体金属 (BM) 具有奥氏体特性。IN 718 BM 基体在镍基体中含有分散的γ′和γ″强化沉淀。另一方面,ASS 304L BM 显示出独特的奥氏体微观结构,具有孪晶特征。焊接金属表现出凝固晶界(SGBs)、迁移晶界(MGBs)和独特的树枝状微观结构,这些都对焊缝的性能产生了影响。通过对 IN 82 焊接区进行大量分析和绘图,发现树枝状间区域含有 Nb、Cr 和 Ti 碳化物。此外,在 IN 82 填充物和焊接区两侧的母材之间还存在未混合区(UZ),表现为岛屿和海滩。利用电子反向散射衍射(EBSD)分析对不同焊接区的纹理进行了评估。此外,通过核平均错位(KAM)显微照片还观察到焊接金属晶粒内部存在明显的应变。根据拉伸试验的结果,在 IN 82 焊接区观察到了断裂,这表明它是 IN 718/ASS 304L 异种焊缝在室温下最薄弱的区域。显微硬度曲线显示焊接区的硬度值很高,这可能是由于出现了不同的显微结构和额外的析出物。在室温下,异种焊接接头的平均拉伸强度为 626 兆帕。此外,还在 550 ℃、600 ℃ 和 650 ℃ 的高温下进行了拉伸强度测量实验。在高温拉伸试验中观察到,与 ASS 304L BM 相比,IN 82 焊接区的拉伸强度更高。有趣的是,304L BM 的高温拉伸试样失败了。夏比冲击韧性测试在 ASS 304L 热影响区、IN 718 热影响区和焊接中心进行。我们使用深孔钻 (DHD) 技术量化了残余应力,并确定了拉伸残余应力最大的位置,发现该位置距离焊接表面 3 毫米。
{"title":"Role of Microstructure Evolution During Welding on Mechanical Properties and Residual Stresses of the Inconel 718 and Austenitic Stainless Steel 304L Dissimilar Weld Joint","authors":"Niraj Kumar, Prakash Kumar, Ravi Shanker Vidyarthy, Chandan Pandey","doi":"10.1007/s11661-024-07571-w","DOIUrl":"https://doi.org/10.1007/s11661-024-07571-w","url":null,"abstract":"<p>For this study, the researchers aimed to dissimilar weld the Nickel-based superalloy Inconel 718 (IN 718) with austenitic stainless steel 304L (ASS 304L) using the gas tungsten arc welding (GTAW) technique and Nickel-based filler IN 82 (ERNiCr-3). In order to examine the weld microstructures, we utilized optical microscopy (OM) and field emission scanning electron microscopy (FESEM) with energy-dispersive spectroscopy (EDS) to identify any segregation present in various weld zones. Through optical and FESEM analyses, it was revealed that the base metals (BM) exhibit an austenitic character. The IN 718 BM matrix contains dispersed <i>γ</i>′ and <i>γ</i>″ strengthening precipitates within the Nickel matrix. On the other hand, the ASS 304L BM displayed a unique austenitic microstructure characterized by twins features. The weld metal exhibited solidification grain boundaries (SGBs), migrated grain boundaries (MGBs), and distinct dendritic microstructures that had an impact on the properties of the weld. Through extensive analysis and mapping of the IN 82 weld zone, it was discovered that interdendritic regions contain carbides of Nb, Cr, and Ti. In addition, there were Unmixed zone (UZ) areas between the IN 82 filler and the base materials on both sides of the weld zone, appearing as islands and beaches. The texture of the different weld zones was evaluated using electron backscattered diffraction (EBSD) analysis. Additionally, the presence of a notable level of strain within the weld metal grains was observed through Kernel average misorientation (KAM) micrographs. Fractures were observed in the IN 82 weld zone, indicating that it is the weakest area in the IN 718/ASS 304L dissimilar weld at room temperature, according to the outputs of the tensile tests. The micro-hardness profile showed substantial hardness values in the weld zone, which can be attributed to the appearance of a diverse microstructure and additional precipitates. At room temperature, the recorded average tensile strength of the dissimilar weld joint was 626 MPa. In addition, experiments were carried out at high temperatures of 550 °C, 600 °C, and 650 °C to measure the tensile strength. In the high-temperature tensile tests, it was observed that the IN 82 weld zone exhibited higher tensile strength compared to the ASS 304L BM. Interestingly, the high temperatures tensile specimens failed in the 304L BM. The Charpy impact toughness test was performed with notches at ASS 304L HAZ, IN 718 HAZ, and the weld center. Using the deep hole drilling (DHD) technique, we were able to quantify residual stress and identify the location of the highest tensile residual stress, which was found to be 3 mm from the weld surface.</p>","PeriodicalId":18504,"journal":{"name":"Metallurgical and Materials Transactions A","volume":"54 1","pages":""},"PeriodicalIF":0.0,"publicationDate":"2024-09-11","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"142177013","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":0,"RegionCategory":"","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}