Poster Unique Formation Characteristics of α’-Martensite in Ti Alloys Processed by Laser Powder Bed Fusion

Yebeen Ji (Graduate School of Frontier Sciences, The University of Tokyo) ; Prince Valentine Cobbinah (Graduate School of Frontier Sciences, The University of Tokyo) ; Yoshiaki Toda SAMURAI ORCID (Center for Basic Research on Materials/Data-driven Materials Research Field/Materials Modeling Group, National Institute for Materials Science) ; Ryosuke Ozasa (Graduate School of Engineering, Osaka University) ; Takuya Ishimoto (University of Toyama) ; Takayoshi Nakano (Graduate School of Engineering, Osaka University) ; Yoko Yamabe-Mitarai (Graduate School of Frontier Sciences, The University of Tokyo)

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Yebeen Ji, Prince Valentine Cobbinah, Yoshiaki Toda, Ryosuke Ozasa, Takuya Ishimoto, Takayoshi Nakano, Yoko Yamabe-Mitarai. Unique Formation Characteristics of α’-Martensite in Ti Alloys Processed by Laser Powder Bed Fusion. https://doi.org/10.48505/nims.5818

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(abstract)

Single and multiple bead tests were conducted on two bulk titanium alloys, (α+β) Ti-6Al-4V (Ti64) and near-α Ti-6Al-2Sn-4Zr-6Mo (Ti6246), to assess the dependence of the melt pool shape and the heat-affected zone on the α'-martensite formation. Although the exact mechanism remains unclear, the results suggest that prolonged thermal exposure plays a critical role. Notably, one alloy showed an a typical α' formation behavior: α' structures became finer with increasing energy density, indicating a unique interplay between alloy composition and localized thermal conditions.

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Keyword: Additive Manufacturing, Powder Bed Fusion,, Ti-6Al-4V, Ti-6Al-2Sn-4Zr-6Mo, volumetric energy density, fast cooling rate, melt pool shape

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Conference: 日本Additive Manufacturing学会 第1回年次講演大会 (2025-09-01 - 2025-09-03)

Funding:

  • 日本学術振興会 21H05198 (超温度場スーパーチタン創成科学)
  • 公益財団法人軽金属奨学会 (教育研究資金・研究補助金)

Manuscript type: Author's version (Submitted manuscript)

MDR DOI: https://doi.org/10.48505/nims.5818

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Updated at: 2025-10-21 16:06:51 +0900

Published on MDR: 2025-10-21 15:43:43 +0900

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