Acta Metallurgica Sinica (English Letters) ›› 2024, Vol. 37 ›› Issue (5): 777-792.DOI: 10.1007/s40195-023-01657-x
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Hasfi F. Nurly1,2, Jinhu Zhang2, Dechun Ren2, Yusheng Cai2, Haibin Ji2(
), Dongsheng Xu1,2, Zhicheng Dong3, Hao Wang3, Qingmiao Hu2, Jiafeng Lei2, Rui Yang1,2,4(
)
Received:2023-06-25
Revised:2023-09-26
Accepted:2023-10-19
Online:2024-05-10
Published:2024-06-14
Contact:
Haibin Ji, hbji@imr.ac.cn; Rui Yang, ryang@imr.ac.cn
Hasfi F. Nurly, Jinhu Zhang, Dechun Ren, Yusheng Cai, Haibin Ji, Dongsheng Xu, Zhicheng Dong, Hao Wang, Qingmiao Hu, Jiafeng Lei, Rui Yang. Refinement of α′ Martensite by Oxygen in Selective Laser Melted Ti-6Al-4V[J]. Acta Metallurgica Sinica (English Letters), 2024, 37(5): 777-792.
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Fig. 1 a Design model, scanning strategies, and as-built material (dimension in mm) of SLMed Ti-6Al-4V. b Morphology of powders and c their size distribution of Ti-6Al-4V-xO
| Alloy | Ti | Al | V | O | Fe | H | C | N | Si |
|---|---|---|---|---|---|---|---|---|---|
| TC4-1 | Bal | 5.86 | 4.18 | 0.11 | 0.032 | 0.0019 | 0.0064 | 0.011 | 0.01 |
| TC4-2 | Bal | 5.85 | 4.18 | 0.16 | 0.027 | 0.0019 | 0.012 | 0.0098 | 0.01 |
| TC4-3 | Bal | 5.85 | 4.16 | 0.21 | 0.026 | 0.0017 | 0.018 | 0.0093 | 0.01 |
| TC4-4 | Bal | 5.95 | 4.16 | 0.25 | 0.022 | 0.0018 | 0.023 | 0.0086 | 0.01 |
Table 1 Chemical compositions of SLMed Ti-6Al-4V-xO alloys (wt%)
| Alloy | Ti | Al | V | O | Fe | H | C | N | Si |
|---|---|---|---|---|---|---|---|---|---|
| TC4-1 | Bal | 5.86 | 4.18 | 0.11 | 0.032 | 0.0019 | 0.0064 | 0.011 | 0.01 |
| TC4-2 | Bal | 5.85 | 4.18 | 0.16 | 0.027 | 0.0019 | 0.012 | 0.0098 | 0.01 |
| TC4-3 | Bal | 5.85 | 4.16 | 0.21 | 0.026 | 0.0017 | 0.018 | 0.0093 | 0.01 |
| TC4-4 | Bal | 5.95 | 4.16 | 0.25 | 0.022 | 0.0018 | 0.023 | 0.0086 | 0.01 |
| Alloy composition (wt%) | △Gβ→α (J/mol) | △GT (J/mol) | △Gsubs (J/mol) | △Gint (J/mol) | Ms (°C) | Tβ (°C) |
|---|---|---|---|---|---|---|
| Ti | 130.861 | 130.861 | 0 | 0 | 845.950 | 882 |
| Ti-1Al | 201.404 | 129.484 | 71.920 | 0 | 848.300 | 909 |
| Ti-2Al | 269.795 | 128.327 | 141.468 | 0 | 849.400 | 933 |
| Ti-3Al | 336.202 | 127.296 | 208.906 | 0 | 849.800 | 956 |
| Ti-4Al | 400.776 | 126.360 | 274.416 | 0 | 849.700 | 976 |
| Ti-5Al | 463.700 | 125.514 | 338.186 | 0 | 849.100 | 996 |
| Ti-6Al | 525.025 | 124.728 | 400.297 | 0 | 848.200 | 1015 |
| Ti-1V | 136.676 | 136.117 | 0.559 | 0 | 813.425 | 863 |
| Ti-2V | 142.599 | 141.436 | 1.162 | 0 | 780.525 | 846 |
| Ti-3V | 148.568 | 146.758 | 1.810 | 0 | 747.625 | 829 |
| Ti-4V | 154.584 | 152.081 | 2.502 | 0 | 714.725 | 813 |
| Ti-6Al-1V | 550.600 | 130.636 | 420.013 | 0 | 809.900 | 996 |
| Ti-6Al-2V | 580.500 | 137.522 | 442.948 | 0 | 765.250 | 978 |
| Ti-6Al-3V | 614.200 | 145.314 | 468.886 | 0 | 714.725 | 959 |
| Ti-1Al-4V | 238.879 | 151.852 | 87.0262 | 0 | 708.850 | 837 |
| Ti-2Al-4V | 322.032 | 151.813 | 170.218 | 0 | 701.800 | 859 |
| Ti-3Al-4V | 404.374 | 151.960 | 252.414 | 0 | 693.575 | 881 |
| Ti-4Al-4V | 486.802 | 152.471 | 334.331 | 0 | 683.000 | 901 |
| Ti-5Al-4V | 569.883 | 153.338 | 416.545 | 0 | 670.075 | 922 |
| Ti-6Al-4V | 652.850 | 154.247 | 498.603 | 0 | 656.800 | 942 |
| Ti-6Al-4V-0.11O | 658.379 | 152.462 | 491.803 | 14.114 | 668.500 | 963 |
| Ti-6Al-4V-0.16O | 660.397 | 151.569 | 488.457 | 20.371 | 674.350 | 973 |
| Ti-6Al-4V-0.21O | 662.981 | 150.826 | 485.600 | 26.555 | 679.225 | 983 |
| Ti-6Al-4V-0.25O | 664.327 | 150.081 | 482.836 | 31.410 | 684.100 | 991 |
Table 2 Chemical driving force of the BCC to HCP structural transformation △Gβ→α, the elastic strain energy △GT, the lattice distortion energy due to substitutional elements △Gsubs and due to interstitial elements △Gint at the martensitic start temperature Ms, and β transus Tβ of Ti-Al-V alloys
| Alloy composition (wt%) | △Gβ→α (J/mol) | △GT (J/mol) | △Gsubs (J/mol) | △Gint (J/mol) | Ms (°C) | Tβ (°C) |
|---|---|---|---|---|---|---|
| Ti | 130.861 | 130.861 | 0 | 0 | 845.950 | 882 |
| Ti-1Al | 201.404 | 129.484 | 71.920 | 0 | 848.300 | 909 |
| Ti-2Al | 269.795 | 128.327 | 141.468 | 0 | 849.400 | 933 |
| Ti-3Al | 336.202 | 127.296 | 208.906 | 0 | 849.800 | 956 |
| Ti-4Al | 400.776 | 126.360 | 274.416 | 0 | 849.700 | 976 |
| Ti-5Al | 463.700 | 125.514 | 338.186 | 0 | 849.100 | 996 |
| Ti-6Al | 525.025 | 124.728 | 400.297 | 0 | 848.200 | 1015 |
| Ti-1V | 136.676 | 136.117 | 0.559 | 0 | 813.425 | 863 |
| Ti-2V | 142.599 | 141.436 | 1.162 | 0 | 780.525 | 846 |
| Ti-3V | 148.568 | 146.758 | 1.810 | 0 | 747.625 | 829 |
| Ti-4V | 154.584 | 152.081 | 2.502 | 0 | 714.725 | 813 |
| Ti-6Al-1V | 550.600 | 130.636 | 420.013 | 0 | 809.900 | 996 |
| Ti-6Al-2V | 580.500 | 137.522 | 442.948 | 0 | 765.250 | 978 |
| Ti-6Al-3V | 614.200 | 145.314 | 468.886 | 0 | 714.725 | 959 |
| Ti-1Al-4V | 238.879 | 151.852 | 87.0262 | 0 | 708.850 | 837 |
| Ti-2Al-4V | 322.032 | 151.813 | 170.218 | 0 | 701.800 | 859 |
| Ti-3Al-4V | 404.374 | 151.960 | 252.414 | 0 | 693.575 | 881 |
| Ti-4Al-4V | 486.802 | 152.471 | 334.331 | 0 | 683.000 | 901 |
| Ti-5Al-4V | 569.883 | 153.338 | 416.545 | 0 | 670.075 | 922 |
| Ti-6Al-4V | 652.850 | 154.247 | 498.603 | 0 | 656.800 | 942 |
| Ti-6Al-4V-0.11O | 658.379 | 152.462 | 491.803 | 14.114 | 668.500 | 963 |
| Ti-6Al-4V-0.16O | 660.397 | 151.569 | 488.457 | 20.371 | 674.350 | 973 |
| Ti-6Al-4V-0.21O | 662.981 | 150.826 | 485.600 | 26.555 | 679.225 | 983 |
| Ti-6Al-4V-0.25O | 664.327 | 150.081 | 482.836 | 31.410 | 684.100 | 991 |
Fig. 3 a Variations of the Gibbs free energy of the β and supersaturated α phase of Ti-6Al-4V containing different levels of oxygen with temperature. Crossings of curves of the two phases are within the area of the rectangle which is enlarged in the inset at the bottom left corner, with the T0 temperatures of the crossings indicated. b Variations of the computed Tβ, T0 and Ms temperatures of Ti-Al-V with oxygen content
Fig. 6 a Schematic illustration of the SLM process showing representative microtexyure maps of SLMed Ti-6Al-4V with β columnar grains (black dashed line) with respect to scan strategy YZ, and b contouring reconstructed orientation pole figures showing growth texture parallel to the build direction
Fig. 7 Microstructure of SLMed Ti–6Al–4V (0.25 wt% oxygen) showing a band contrast with CSL component defined $\left[ {11\overline{2}0} \right]$ intervariant misorientation of twin boundaries, neighboring random β phase. b Contouring component analysis of $\left\{ {10\overline{1}1} \right\}$ pole figure, c bright field image $,$ d dark field image of an α′ lath $,$ with selected area electron diffraction patterns of e the α′ phase and f the β phase.
| (hkl) | [uvw] | θ (°) |
|---|---|---|
| - | ||
| 0 | ||
| 90 | ||
| 90 | ||
| 8.1 | ||
| 8.1 | ||
| 81.9 | ||
| 81.9 | ||
| 8.1 | ||
| 8.1 | ||
| 81.9 | ||
| 81.9 | ||
| - | ||
| 0 | ||
| 73.7 | ||
| 73.7 | ||
| 16.3 | ||
| 16.3 | ||
| 90 | ||
| 90 | ||
| 8.1 | ||
| 8.1 | ||
| 81.9 | ||
| 81.9 |
Table 3 Martensite habit planes (hkl), its traces [uvw] on (001), and the angle (θ) between [uvw] and $\left[ {1\overline{1}0} \right]$ (the trace line of (334) habit plane), or between [uvw] and $\left[ {4\overline{3}0} \right]$ (the trace line of (344) habit plane)
| (hkl) | [uvw] | θ (°) |
|---|---|---|
| - | ||
| 0 | ||
| 90 | ||
| 90 | ||
| 8.1 | ||
| 8.1 | ||
| 81.9 | ||
| 81.9 | ||
| 8.1 | ||
| 8.1 | ||
| 81.9 | ||
| 81.9 | ||
| - | ||
| 0 | ||
| 73.7 | ||
| 73.7 | ||
| 16.3 | ||
| 16.3 | ||
| 90 | ||
| 90 | ||
| 8.1 | ||
| 8.1 | ||
| 81.9 | ||
| 81.9 |
Fig. 8 Four SEM images of Fig. 5a, with trace lines of martensite plates marked, and typical angles between these trace lines numbered from 1 to 12. A prior β grain boundary running down the middle of the second image is indicated by a dotted line
| Angle | Value (°) | θ (°) |
|---|---|---|
| 1 | 7 | 8.1 |
| 2 | 13 | 16.3 |
| 3 | 90 | 90 |
| 4 | 70 | 73.7 |
| 5 | 90 | 90 |
| 6 | 75 | 73.7 |
| 7 | 70 | 73.7 |
| 8 | 68 | 73.7 |
| 9 | 9 | 8.1 |
| 10 | 70 | 73.7 |
| 11 | 72 | 73.7 |
| 12 | 73 | 73.7 |
Table 4 Measured values of the angle number 1 to 12 marked on the SEM images of Fig. 8, together with the closest theoretical value of θ between traces of habit planes as listed in Table 3
| Angle | Value (°) | θ (°) |
|---|---|---|
| 1 | 7 | 8.1 |
| 2 | 13 | 16.3 |
| 3 | 90 | 90 |
| 4 | 70 | 73.7 |
| 5 | 90 | 90 |
| 6 | 75 | 73.7 |
| 7 | 70 | 73.7 |
| 8 | 68 | 73.7 |
| 9 | 9 | 8.1 |
| 10 | 70 | 73.7 |
| 11 | 72 | 73.7 |
| 12 | 73 | 73.7 |
Fig. 9 Average thickness (width) and length of the first generation of α′ martensite plates based on measurements on SEM images taken from a XY planes and b YZ planes
| Alloy | Al | V | O |
|---|---|---|---|
| TC4-1 | 3.809 | 1.7556 | 2.09 |
| TC4-2 | 3.8025 | 1.7556 | 3.04 |
| TC4-3 | 3.8025 | 1.7472 | 3.990001 |
| TC4-4 | 3.8675 | 1.7472 | 4.750001 |
Table 5 Calculated growth restriction factors Q of different alloying additions in the investigated Ti-6Al-4V alloys
| Alloy | Al | V | O |
|---|---|---|---|
| TC4-1 | 3.809 | 1.7556 | 2.09 |
| TC4-2 | 3.8025 | 1.7556 | 3.04 |
| TC4-3 | 3.8025 | 1.7472 | 3.990001 |
| TC4-4 | 3.8675 | 1.7472 | 4.750001 |
Fig. 10 Analysis of intervariant crystallographic plane distribution of martensite in SLMed Ti-6Al-4V with different oxygen content: a inverse pole figure (IPF) maps, b contour plot of intervariant misorientation axis I, c contour plot of intervariant misorientation axes II + III, and d intensity distribution of specific disorientation angles associated with the Burgers orientation relationship for the alloy containing 0.25% oxygen, with the range of misorientation angle indicated
Fig. 12 a Schematic thermal cycle illustration showing b proposed phase transformation pathway of α′ martensite refinement during SLM processing of Ti-6Al-4V
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