From macro-, through meso- to micro-scale: Densification behavior, deformation response and microstructural evolution of selective laser melted Mg-RE alloy
Cheng Chang, Guangrui Yao, Sophie C. Cox, Xiaofeng Zhang, Liyuan Sheng, Min Liu, Weili Cheng, Yang Lu, Xingchen Yan
{"title":"From macro-, through meso- to micro-scale: Densification behavior, deformation response and microstructural evolution of selective laser melted Mg-RE alloy","authors":"Cheng Chang, Guangrui Yao, Sophie C. Cox, Xiaofeng Zhang, Liyuan Sheng, Min Liu, Weili Cheng, Yang Lu, Xingchen Yan","doi":"10.1016/j.jma.2024.12.018","DOIUrl":null,"url":null,"abstract":"To clarify the densification behavior, deformation response and strengthening mechanisms of selective laser melted (SLM) Mg-RE alloys, this study systematically investigates a representative WE43 alloy via advanced material characterization techniques. A suitable laser output mode fell into the transition mode, allowing for the fabrication of nearly full-density samples (porosity = 0.85 ± 0.021 %) with favorable mechanical properties (yield strength=351 MPa, ultimate tensile strength = 417 MPa, the elongation at break = 6.5 % and microhardness = 137.9 ± 6.15 HV<sub>0.1</sub>) using optimal processing parameters (<em>P</em> = 80 W, <em>v</em> = 250 mm/s and <em>d</em> = 50 µm). Viscoplastic self-consistent analysis and transmission electron microscopy observations reveal that the plastic deformation response of the SLM Mg-RE alloys is primarily driven by basal <<em>a</em>> and prismatic <<em>a</em>> slips. Starting from a random texture before deformation (maximum multiple of ultimate density, Max. MUD = 3.95), plastic stretching led the grains to align with the Z-axis, finally resulting in a {0001}<<span><span style=\"\"></span><span data-mathml='<math xmlns=\"http://www.w3.org/1998/Math/MathML\"><mrow is=\"true\"><mn is=\"true\">10</mn><mover accent=\"true\" is=\"true\"><mn is=\"true\">1</mn><mo is=\"true\">&#xAF;</mo></mover><mn is=\"true\">0</mn></mrow></math>' role=\"presentation\" style=\"font-size: 90%; display: inline-block; position: relative;\" tabindex=\"0\"><svg aria-hidden=\"true\" focusable=\"false\" height=\"2.202ex\" role=\"img\" style=\"vertical-align: -0.235ex;\" viewbox=\"0 -846.5 2072 947.9\" width=\"4.812ex\" xmlns:xlink=\"http://www.w3.org/1999/xlink\"><g fill=\"currentColor\" stroke=\"currentColor\" stroke-width=\"0\" transform=\"matrix(1 0 0 -1 0 0)\"><g is=\"true\"><g is=\"true\"><use xlink:href=\"#MJMAIN-31\"></use><use x=\"500\" xlink:href=\"#MJMAIN-30\" y=\"0\"></use></g><g is=\"true\" transform=\"translate(1001,0)\"><g is=\"true\" transform=\"translate(35,0)\"><use xlink:href=\"#MJMAIN-31\"></use></g><g is=\"true\" transform=\"translate(0,198)\"><use x=\"-70\" xlink:href=\"#MJMAIN-AF\" y=\"0\"></use><use x=\"70\" xlink:href=\"#MJMAIN-AF\" y=\"0\"></use></g></g><g is=\"true\" transform=\"translate(1571,0)\"><use xlink:href=\"#MJMAIN-30\"></use></g></g></g></svg><span role=\"presentation\"><math xmlns=\"http://www.w3.org/1998/Math/MathML\"><mrow is=\"true\"><mn is=\"true\">10</mn><mover accent=\"true\" is=\"true\"><mn is=\"true\">1</mn><mo is=\"true\">¯</mo></mover><mn is=\"true\">0</mn></mrow></math></span></span><script type=\"math/mml\"><math><mrow is=\"true\"><mn is=\"true\">10</mn><mover accent=\"true\" is=\"true\"><mn is=\"true\">1</mn><mo is=\"true\">¯</mo></mover><mn is=\"true\">0</mn></mrow></math></script></span>> texture orientation after fracture (Max. MUD = 8.755). Main phases of the SLM state are mainly composed of α-Mg, Mg<sub>24</sub>Y<sub>5</sub> and β’-Mg<sub>41</sub>Nd<sub>5</sub>, with an average grain size of only 4.27 µm (about a quarter of that in the extruded state), resulting in a favorable strength-toughness ratio. Except for the nano-β’ phase and semi-coherent Mg<sub>24</sub>Y<sub>5</sub> phase (mismatch = 16.12 %) around the grain boundaries, a small amount of nano-ZrO<sub>2</sub> and Y<sub>2</sub>O<sub>3</sub> particles also play a role in dispersion strengthening. The high mechanical properties of the SLM state are chiefly attributed to precipitation hardening (44.41 %), solid solution strengthening (34.06 %) and grain boundary strengthening (21.53 %), with precipitation hardening being predominantly driven by dislocation strengthening (67.77 %). High-performance SLM Mg-RE alloy components were manufactured and showcased at TCT Asia 2024, receiving favorable attention. This work underscores the significant application potential of SLM Mg-RE alloys and establishes a strong foundation for advancing their use in the biomedical fields.","PeriodicalId":16214,"journal":{"name":"Journal of Magnesium and Alloys","volume":"8 1","pages":""},"PeriodicalIF":15.8000,"publicationDate":"2025-01-17","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":"0","resultStr":null,"platform":"Semanticscholar","paperid":null,"PeriodicalName":"Journal of Magnesium and Alloys","FirstCategoryId":"88","ListUrlMain":"https://doi.org/10.1016/j.jma.2024.12.018","RegionNum":1,"RegionCategory":"材料科学","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"","PubModel":"","JCR":"Q1","JCRName":"METALLURGY & METALLURGICAL ENGINEERING","Score":null,"Total":0}
引用次数: 0
Abstract
To clarify the densification behavior, deformation response and strengthening mechanisms of selective laser melted (SLM) Mg-RE alloys, this study systematically investigates a representative WE43 alloy via advanced material characterization techniques. A suitable laser output mode fell into the transition mode, allowing for the fabrication of nearly full-density samples (porosity = 0.85 ± 0.021 %) with favorable mechanical properties (yield strength=351 MPa, ultimate tensile strength = 417 MPa, the elongation at break = 6.5 % and microhardness = 137.9 ± 6.15 HV0.1) using optimal processing parameters (P = 80 W, v = 250 mm/s and d = 50 µm). Viscoplastic self-consistent analysis and transmission electron microscopy observations reveal that the plastic deformation response of the SLM Mg-RE alloys is primarily driven by basal <a> and prismatic <a> slips. Starting from a random texture before deformation (maximum multiple of ultimate density, Max. MUD = 3.95), plastic stretching led the grains to align with the Z-axis, finally resulting in a {0001}<> texture orientation after fracture (Max. MUD = 8.755). Main phases of the SLM state are mainly composed of α-Mg, Mg24Y5 and β’-Mg41Nd5, with an average grain size of only 4.27 µm (about a quarter of that in the extruded state), resulting in a favorable strength-toughness ratio. Except for the nano-β’ phase and semi-coherent Mg24Y5 phase (mismatch = 16.12 %) around the grain boundaries, a small amount of nano-ZrO2 and Y2O3 particles also play a role in dispersion strengthening. The high mechanical properties of the SLM state are chiefly attributed to precipitation hardening (44.41 %), solid solution strengthening (34.06 %) and grain boundary strengthening (21.53 %), with precipitation hardening being predominantly driven by dislocation strengthening (67.77 %). High-performance SLM Mg-RE alloy components were manufactured and showcased at TCT Asia 2024, receiving favorable attention. This work underscores the significant application potential of SLM Mg-RE alloys and establishes a strong foundation for advancing their use in the biomedical fields.
期刊介绍:
The Journal of Magnesium and Alloys serves as a global platform for both theoretical and experimental studies in magnesium science and engineering. It welcomes submissions investigating various scientific and engineering factors impacting the metallurgy, processing, microstructure, properties, and applications of magnesium and alloys. The journal covers all aspects of magnesium and alloy research, including raw materials, alloy casting, extrusion and deformation, corrosion and surface treatment, joining and machining, simulation and modeling, microstructure evolution and mechanical properties, new alloy development, magnesium-based composites, bio-materials and energy materials, applications, and recycling.