Junjie Shi, Sheng Li, Chenglin Kang, Futong Li, Min Chen, Shizhuo Yin, Jianzhong Li
This study presents the first systematic experimental determination of phase equilibria in the Er2O3–Al2O3–SiO2 system at 1600°C in air, employing the high-temperature isothermal equilibration method followed by rapid drop-quenching to preserve high-temperature phase assemblages. The mineralogy and chemical compositions of the equilibrated samples were analyzed by x-ray diffraction (XRD), scanning electron microscopy (SEM), and electron probe x-ray microanalysis (EPMA). One single liquid equilibria, five two-phase equilibria (liquid–SiO2, liquid–Er2Si2O7, liquid–Er3Al5O12, liquid–Al2O3, and liquid–mullite) and seven three-phase equilibria (liquid–SiO2–Er2Si2O7, liquid–Er2Si2O7–Er2SiO5, liquid–Er2SiO5–Er3Al5O12, liquid–Er3Al5O12–Al2O3, liquid–Al2O3–mullite, Er2O3–Er2SiO5–Er4Al2O9, Er3Al5O12–Er2SiO5–Er4Al2O9) were observed in the equilibrium ternary system. The 1600°C isothermal section of the Er2O3–Al2O3–SiO2 phase diagram in air (pO2 = 0.21 atm) was constructed based on the present experimentally determined equilibrium phase compositions. The liquid area and the primary fields of SiO2, Er2Si2O7, Er3Al5O12, Al2O3, and mullite were constructed. The comparison of the present experimental results deviate significantly from the modelling by FactSage (version 8.3) using its “FactPS” and “FToxid” databases, suggesting that FactSage underestimated the stability of the liquid phase under the present experimental conductions.
{"title":"Phase equilibria of the Er2O3–Al2O3–SiO2 system at 1600°C related to corrosion of environmental barrier coatings","authors":"Junjie Shi, Sheng Li, Chenglin Kang, Futong Li, Min Chen, Shizhuo Yin, Jianzhong Li","doi":"10.1111/jace.70416","DOIUrl":"https://doi.org/10.1111/jace.70416","url":null,"abstract":"<p>This study presents the first systematic experimental determination of phase equilibria in the Er<sub>2</sub>O<sub>3</sub>–Al<sub>2</sub>O<sub>3</sub>–SiO<sub>2</sub> system at 1600°C in air, employing the high-temperature isothermal equilibration method followed by rapid drop-quenching to preserve high-temperature phase assemblages. The mineralogy and chemical compositions of the equilibrated samples were analyzed by x-ray diffraction (XRD), scanning electron microscopy (SEM), and electron probe x-ray microanalysis (EPMA). One single liquid equilibria, five two-phase equilibria (liquid–SiO<sub>2</sub>, liquid–Er<sub>2</sub>Si<sub>2</sub>O<sub>7</sub>, liquid–Er<sub>3</sub>Al<sub>5</sub>O<sub>12</sub>, liquid–Al<sub>2</sub>O<sub>3</sub>, and liquid–mullite) and seven three-phase equilibria (liquid–SiO<sub>2</sub>–Er<sub>2</sub>Si<sub>2</sub>O<sub>7</sub>, liquid–Er<sub>2</sub>Si<sub>2</sub>O<sub>7</sub>–Er<sub>2</sub>SiO<sub>5</sub>, liquid–Er<sub>2</sub>SiO<sub>5</sub>–Er<sub>3</sub>Al<sub>5</sub>O<sub>12</sub>, liquid–Er<sub>3</sub>Al<sub>5</sub>O<sub>12</sub>–Al<sub>2</sub>O<sub>3</sub>, liquid–Al<sub>2</sub>O<sub>3</sub>–mullite, Er<sub>2</sub>O<sub>3</sub>–Er<sub>2</sub>SiO<sub>5</sub>–Er<sub>4</sub>Al<sub>2</sub>O<sub>9</sub>, Er<sub>3</sub>Al<sub>5</sub>O<sub>12</sub>–Er<sub>2</sub>SiO<sub>5</sub>–Er<sub>4</sub>Al<sub>2</sub>O<sub>9</sub>) were observed in the equilibrium ternary system. The 1600°C isothermal section of the Er<sub>2</sub>O<sub>3</sub>–Al<sub>2</sub>O<sub>3</sub>–SiO<sub>2</sub> phase diagram in air (<i>p</i>O<sub>2</sub> = 0.21 atm) was constructed based on the present experimentally determined equilibrium phase compositions. The liquid area and the primary fields of SiO<sub>2</sub>, Er<sub>2</sub>Si<sub>2</sub>O<sub>7</sub>, Er<sub>3</sub>Al<sub>5</sub>O<sub>12</sub>, Al<sub>2</sub>O<sub>3</sub>, and mullite were constructed. The comparison of the present experimental results deviate significantly from the modelling by FactSage (version 8.3) using its “<i>FactPS</i>” and “<i>FToxid</i>” databases, suggesting that FactSage underestimated the stability of the liquid phase under the present experimental conductions.</p>","PeriodicalId":200,"journal":{"name":"Journal of the American Ceramic Society","volume":"109 1","pages":""},"PeriodicalIF":3.8,"publicationDate":"2025-12-05","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"145695250","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":3,"RegionCategory":"材料科学","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
Qinqin Xu, Ibrahim Goda, Agata Zaborowska, Katarzyna Mulewska, Witold Chrominski, Damian Kalita, Łukasz Kurpaska, Claudio Fusco, Fabrizio Rovaris, Wenyi Huo
Brittle oxides, such as α-Al2O3, i.e., sapphire, are traditionally unsuitable for ductile applications, yet exhibit enhanced plasticity at nanoscale. This study explores the mechanical behavior of c-plane-oriented, dislocation-free monocrystalline α-Al2O3 via molecular dynamics (MD) simulations and experiments, including nanoindentation and post-indentation TEM analysis. The results demonstrate high strength with homogeneous, extensive deformation without failure. Plasticity is dominated by basal (0001) dislocations and rhombohedral [10