Formation of (Ti,W)Fe2 C14 laves phase in the W-Ti-Fe system and the impact on mechanical properties

Tungsten-based alloys utilising coherent intermetallic strengthening offer a route to improved high temperature strength. Recently proposed W-Ti-Fe alloys employ B2 TiFe phase in an A2 BCC matrix to achieve this strengthening, however, other phases such as the TiFe 2 Laves phase can form at higher temperatures. In this study, the formation of the (Ti,W)Fe 2 C14 phase in a BCC W-rich matrix is observed in a W–16Ti–4Fe (at.%) alloy produced by vacuum arc-melting and annealing at 1400 o C. There was no evidence for the formation of either the TiFe B2 or W 6 Fe 7 μ phase from analysis of the TEM diffraction patterns. The C14 Laves phase was found to have a composition of 8.8 ± 0.2 W, 23.3 ± 0.2Ti and 68.0 ± 0.8Fe (at.%) consistent with (Ti,W)Fe 2 . This formed a continuous region along the boundaries between the W-rich BCC prior-dendrites, as well as in smaller isolated precipitates. The prior dendritic regions consisted of W-rich BCC phase with a composition of 84.10±0.41 W, 13.94 ± 0.73Ti and 1.94 ± 0.73Fe (at.%). Thermodynamic calculations using CALPHAD predicted the formation of a W rich BCC phase and a Ti and Fe rich liquid phase initially, which was not consistent with the presented experimental findings. A revised calculation which reduced the stability of the μ phase at high temperatures led to an improved prediction, consistent with the experimental results. To investigate the mechanical impact of the C14 phase, a combination of Continuous Stiffness Measurement (CSM) nanoindentation and high-speed nanoindentation mapping was used to measure the comparative hardness of the matrix and precipitate phases, which showed that the C14 phase exhibits a very high hardness relative to the W-rich matrix phase. An average nanohardness of 6.25 ± 0.03 GPa was measured at depth of 1.5 μm using CSM nanoindentation, which is higher than comparable B2 reinforced WTiFe alloys. • A W-16Ti-4Fe (at.%) alloy heated at 1400 o C formed a (W,Ti)Fe 2 C14 phase • A revised prediction of the W-Ti-Fe system agreed with experimental analysis • The relative stability of the μ-phase was reduced at 1400 o C to improve prediction • Nanoindentation mapping showed the C14 phase has a higher hardness than the matrix

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Journal
Journal of Alloys and Compounds
Published
2026-01-13
DOI
https://doi.org/10.1016/j.jallcom.2026.186169
Primary Topic
Advanced materials and composites
Type
article
Field-Weighted Citation Impact
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article

Formation of (Ti,W)Fe2 C14 laves phase in the W-Ti-Fe system and the impact on mechanical properties

Kan Ma, Andrew London, Matthew J. Lloyd, Alexander J. Knowles et al.
Journal of Alloys and Compounds
Advanced materials and composites
article

Formation of (Ti,W)Fe2 C14 laves phase in the W-Ti-Fe system and the impact on mechanical properties

Kan Ma, Andrew London, Matthew J. Lloyd, Alexander J. Knowles, James Gibson, Chris Hardie, Andy Watson
article en

Abstract

Tungsten-based alloys utilising coherent intermetallic strengthening offer a route to improved high temperature strength. Recently proposed W-Ti-Fe alloys employ B2 TiFe phase in an A2 BCC matrix to achieve this strengthening, however, other phases such as the TiFe 2 Laves phase can form at higher temperatures. In this study, the formation of the (Ti,W)Fe 2 C14 phase in a BCC W-rich matrix is observed in a W–16Ti–4Fe (at.%) alloy produced by vacuum arc-melting and annealing at 1400 o C. There was no evidence for the formation of either the TiFe B2 or W 6 Fe 7 μ phase from analysis of the TEM diffraction patterns. The C14 Laves phase was found to have a composition of 8.8 ± 0.2 W, 23.3 ± 0.2Ti and 68.0 ± 0.8Fe (at.%) consistent with (Ti,W)Fe 2 . This formed a continuous region along the boundaries between the W-rich BCC prior-dendrites, as well as in smaller isolated precipitates. The prior dendritic regions consisted of W-rich BCC phase with a composition of 84.10±0.41 W, 13.94 ± 0.73Ti and 1.94 ± 0.73Fe (at.%). Thermodynamic calculations using CALPHAD predicted the formation of a W rich BCC phase and a Ti and Fe rich liquid phase initially, which was not consistent with the presented experimental findings. A revised calculation which reduced the stability of the μ phase at high temperatures led to an improved prediction, consistent with the experimental results. To investigate the mechanical impact of the C14 phase, a combination of Continuous Stiffness Measurement (CSM) nanoindentation and high-speed nanoindentation mapping was used to measure the comparative hardness of the matrix and precipitate phases, which showed that the C14 phase exhibits a very high hardness relative to the W-rich matrix phase. An average nanohardness of 6.25 ± 0.03 GPa was measured at depth of 1.5 μm using CSM nanoindentation, which is higher than comparable B2 reinforced WTiFe alloys. • A W-16Ti-4Fe (at.%) alloy heated at 1400 o C formed a (W,Ti)Fe 2 C14 phase • A revised prediction of the W-Ti-Fe system agreed with experimental analysis • The relative stability of the μ-phase was reduced at 1400 o C to improve prediction • Nanoindentation mapping showed the C14 phase has a higher hardness than the matrix

Journal of Alloys and CompoundsVol. 1055
City University of Hong Kong (HK), European Thermodynamics (United Kingdom) (GB), United Kingdom Atomic Energy Authority (GB), University of Birmingham (GB)
UK Research and Innovation, Henry Royce Institute, Royal Academy of Engineering, Division of Materials Research
Openalex Percentile: Top 89%
Advanced materials and composites
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