Metastable phase and microstructural degradation of a TiAl alloy produced via selective electron beam melting
Introduction
TiAl alloys are promising high-temperature structural material in the aerospace field due to their low density, excellent specific strength, good oxidation resistance and excellent creep properties at elevated temperature [[1], [2], [3]]. However, their low room-temperature ductility and poor deformability make it difficult to form complex shapes and limit their extensive applications [4,5].
Many solutions have been suggested to overcome these limitations, including additive manufacturing, or three-dimensional printing technology, which has gained increased attention [[6], [7], [8], [9]]. Selective electron beam melting (SEBM), as an additive manufacturing technique, has a relatively high preheating temperature, which can reduce the residual stress and avoid crack generation, and is considered a suitable method for manufacturing TiAl alloy components [10,11].
The lamellar structure of the TiAl alloy is unstable and degrades above 800 °C [[12], [13], [14]]. The SEBM technique was characterized by layer upon layer to make parts from 3D model data. Phase transformations and the in-situ decomposition of lamellar colonies has resulted in as-built samples based on the SEBM characteristics because of the high preheating temperature (>1000 °C) and the cycle heating and cooling during SEBM. Some studies reported that lamellar structure degradation deteriorated the TiAl alloy mechanical properties [15,16]. Yang et al. [16] investigated the SEBM-produced titanium alloy microstructure and found that an inhomogeneous microstructure resulted along the building direction because of the difference in thermal history for each power layer. Various degradation methods of lamellar structure exist at elevated temperature, which play an important role on microstructural evolution and mechanical properties.
Previous studies indicated that the SEBM process parameters had an important effect on the microstructure and mechanical properties of the SEBM-produced TiAl alloy, and the microstructure transformed from a fine duplex structure to a γ/B2 structure when the energy density increased [17]. Therefore, the phase transformation and microstructural evolution during SEBM were related closely to the process parameters because the process parameters affected the thermal history of the SEBM-produced TiAl alloy samples. Different SEBM process parameters resulted in different heat inputs and thermal histories, which led to different phase transformations and microstructural evolutions. SEBM-produced TiAl alloys with a fine duplex structure exhibited excellent mechanical properties when the energy density input was 20.04 J/mm3 [17]. Chen et al. [18] investigated the phase transformation and microstructural evolution of TiAl alloys during SEBM when the energy density was 24.07 J/mm3.
To the authors’ best knowledge, the intrinsic heat treatment in the SEBM process is critical in the final phase composition. There is a lack of systematic research on the phase transformation at a low energy density during SEBM. Limited information exists on the microstructural degradation mechanism of a lamellar colony of the SEBM-produced TiAl alloy, which made it challenging to achieve fine control of the target performance. Therefore, the phase transformation and degradation mechanism of a lamellar colony of the SEBM-produced TiAl alloy sample that was fabricated at a low energy density should be elucidated.
In this work, a Ti–47Al–2Cr–2Nb alloy was fabricated via SEBM at a low energy density and the SEBM-produced sample microstructure at different heights was characterized. The phase transformation and microstructural degradation mechanism were investigated and the formation mechanism of a metastable Ti2Al phase was discussed. Finally, the degradation mechanism of a lamellar colony was discussed in detail.
Section snippets
SEBM process
SEBM experiments were carried out on an Arcam A2XX system under a vacuum of 1 × 10−3 mbar. Cubes measuring 20 mm × 20 mm × 20 mm were built on a stainless-steel substrate by SEBM with a nominal composition of Ti–47Al–2Cr–2Nb (at. %) gas-atomized powder particles. During SEBM, scanning was conducted in a snake-like manner with a 90° rotation between adjacent layers. The process parameters as selected based on previous experiments were: beam current = 5.5 mA, scanning speed = 2100 mm s−1, layer
Microstructure at different heights
Fig. 2 shows the SEM and TEM images of the microstructure in transverse cross-section at different heights. The microstructure of sample S1 in the top surface exhibited a near fully lamellar colony with a fine lamellar spacing, as shown in Fig. 2(a), and the length was 10 nm by statistical analysis. The microstructure at the height of 19 mm was observed and equiaxed γ phase and a few B2 phases precipitated within (α2/γ) lamellar colonies and on colony boundaries, as shown in Fig. 2(b). As the
Conclusions
A Ti–47Al–2Cr–2Nb alloy was fabricated by selective electron beam melting. The microstructure, phase transformation and microhardness were investigated. The main conclusions were the following.
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The starting microstructure after solidification in the top surface exhibited a near-fully lamellar structure, whereas the microstructure degraded and displayed a fine duplex structure in the middle and bottom parts. The microstructure in the middle and bottom portions experienced rapid heating and
Data availability
All data included in this study are available upon request by contact with the corresponding author.
Declaration of competing interest
The authors declare that they have no known competing financial interests or personal relationships that could have appeared to influence the work reported in this paper.
Acknowledgements
This work was financially supported by Natural Science Research Projects in Universities of Jiangsu Province (Project No. 20KJB430014). This work was also financially supported by the National Natural Science Foundation of China (Project No. 52001143, No. 51831001 and No. 52075228). This research was funded by the Natural Science Foundation of Jiangsu Province (No. BK20191458), the Natural Science Foundation for Higher Education of Jiangsu Province (No. 20KJA430001) and the Key Research and
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