{101ˉ2}孪晶,全马氏体," /> {101ˉ2}孪晶,全马氏体,"/> {101ˉ2} twin,full martensite,"/> <strong>TC4</strong>钛合金激光表面重熔层内拉伸变形$\{10\bar{1}2\}$孪晶形成机制及马氏体变体选择规律
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金属学报  2026, Vol. 62 Issue (9): 1517-1527    DOI: 10.11900/0412.1961.2024.00286
  研究论文 本期目录 | 过刊浏览 |
TC4钛合金激光表面重熔层内拉伸变形$\{10\bar{1}2\}$孪晶形成机制及马氏体变体选择规律
杨朋飞1(), 孙磊1, 孙奇2, 杨志远3, 赵元1, 高英1, 张嘉振4
1 浙江师范大学 工学院 金华 321004
2 西南交通大学 材料科学与工程学院 材料先进技术教育部重点实验室 成都 610036
3 中材高新氮化物陶瓷有限公司 淄博 255000
4 中国商用飞机有限责任公司北京民用飞机技术研究中心 北京 102200
Formation Mechanism of $\{10\bar{1}2\}$ Twins and Selection Rule of Martensitic Variants During Tensile Deformation in TC4 Titanium Alloy Laser Surface Remelting Layer
YANG Pengfei1(), SUN Lei1, SUN Qi2, YANG Zhiyuan3, ZHAO Yuan1, GAO Ying1, ZHANG Jiazhen4
1 College of Engineering, Zhejiang Normal University, Jinhua 321004, China
2 Key Laboratory of Advanced Technologies of Materials (Ministry of Education), School of Materials Science and Engineering, Southwest Jiaotong University, Chengdu 610036, China
3 Sinoma Advanced Nitride Ceramics Co. Ltd., Zibo 255000, China
4 Beijing Aeronautical Science and Technology Research Institute of COMAC, Beijing 102200, China
引用本文:

杨朋飞, 孙磊, 孙奇, 杨志远, 赵元, 高英, 张嘉振. TC4钛合金激光表面重熔层内拉伸变形$\{10\bar{1}2\}$孪晶形成机制及马氏体变体选择规律[J]. 金属学报, 2026, 62(9): 1517-1527.
Pengfei YANG, Lei SUN, Qi SUN, Zhiyuan YANG, Yuan ZHAO, Ying GAO, Jiazhen ZHANG. Formation Mechanism of $\{10\bar{1}2\}$ Twins and Selection Rule of Martensitic Variants During Tensile Deformation in TC4 Titanium Alloy Laser Surface Remelting Layer[J]. Acta Metall Sin, 2026, 62(9): 1517-1527.

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摘要: 

激光表面重熔(LSR)技术能够显著提升TC4钛合金的力学性能。深入研究LSR过程中TC4钛合金的显微组织演变规律及其对后续拉伸变形机制的影响,对于进一步优化 LSR 工艺至关重要。本工作在全马氏体TC4试样的正面和背面进行LSR处理,随后开展拉伸实验,利用TEM和EBSD技术分析了材料在拉伸过程中的微观结构演变,特别是{101¯2}孪晶的形成及其分布特征。结果表明,在LSR过程中,激光快速冷却特性显著诱发了残余应力,该效应不仅促进了特定型马氏体变体的优先生成,还降低了孪晶开启所需的临界分切应力;同时,激光处理时Al元素的蒸发降低了材料的轴比c / a,减弱了晶格的各向异性,进一步促进了{101¯2}孪晶的形成。孪晶主要集中于几种具有特定取向的马氏体变体中,这些变体在快速冷却条件下显示出明显的择优生成趋势。

关键词 : TC4钛合金,  激光表面重熔,  异质结构,  {101ˉ2}孪晶')" href="#">{101ˉ2}孪晶,  全马氏体    
Abstract:

Laser surface remelting (LSR) technology significantly enhances the mechanical properties of the TC4 titanium alloy. A comprehensive investigation into the microstructural evolution of TC4 alloy during LSR and its effects on subsequent tensile deformation mechanism is essential for optimizing LSR. In this study, LSR treatment was applied to both the front and back of full martensitic TC4 specimens, followed by tensile testing. TEM and EBSD were used to analyze the microstructural evolution during tensile deformation, focusing on the formation and distribution characteristics of {101¯2} twins. The results show that rapid cooling during LSR induces significant residual stress. This in turn not only promotes the preferential formation of specific martensite variants but also lowers the critical shear stress required for twinning. In addition, the evaporation of aluminum during laser treatment decreases the c / a ratio of the TC4 alloy, weakens the anisotropy of the crystal lattice, and further promotes the formation of {101¯2} twins. These twins are primarily concentrated in several martensite variants with specific orientations, exhibiting a clear tendency for preferential formation under rapid cooling conditions.

Key words: TC4 titanium alloy    laser surface remelting    heterostructure    {101ˉ2} twin')" href="#">{101ˉ2} twin    full martensite
收稿日期: 2024-08-19     
ZTFLH:  TG178  
基金资助:国家自然科学基金项目(52475219);中央高校基本科研业务费项目(2682023ZTPY006);中央高校基本科研业务费项目(2682024GF00);四川省自然科学基金项目(2023NSFSC0411)
通讯作者: 杨朋飞,yangpf@zjnu.edu.cn,主要从事增材制造钛合金的组织和性能研究
Corresponding author: YANG Pengfei, Tel: 15608083713, E-mail: yangpf@zjnu.edu.cn
作者简介: 杨朋飞,男,1996年生,博士
图1  水淬-激光表面重熔(WQ-LSR)试样断口附近重熔层的EBSD表征结果
图2  WQ-LSR试样断口表面{101¯2}孪晶TEM像及选区电子衍射花样
图3  WQ-LSR试样拉伸断口EBSD取向分析
Matrix orientation in Euler angle / (°)Twin typeTwin orientation in Euler angle / (°)Twin variant
(93.7, 91.4, 45.0)T1(9.2, 74.2, 55.8)(1¯102)[11¯01]
T2(178.6, 105.1, 0.0)(11¯02)[1¯101]
T4(9.8, 134.9, 3.4)(1¯012)[101¯1]
T5(168.5,164.6, 45.7)(01¯12)[011¯1]
T6(32.7, 16.0, 30.6)(011¯2)[01¯11]
表1  图3a中孪晶变体的分析结果
图4  WQ-LSR试样柱面滑移和基面滑移的Schmid因子分布图及统计图
图5  WQ试样柱面滑移和基面滑移的SF分布图及统计图
SampleAlTiV
WQ6.7289.763.52
WQ-LSR5.74 (-14.58%)90.63 (+0.96%)3.63 (+3.13%)
表2  WQ和WQ-LSR试样的STEM-EDS元素分析结果 (mass fraction / %)
VariantPlane parallelDirection parallelRotation angle/axis from V1
V111¯0β//0001α111β//112¯0α-
V211¯0β//0001α111¯β//112¯0α10.53°/0001
V3110β//0001α11¯1β//112¯0α90°/1 2.38¯ 1.38 0
V4110β//0001α1¯11β//112¯0α90°/1 2.38¯ 1.38 0
V5101¯β//0001α11¯1β//112¯0α60.83°/1.377¯ 1 2.377 0.359
V6101¯β//0001α111β//112¯0α60°/112¯0
V7011¯β//0001α1¯11β//112¯0α60.83°/1.377¯ 1 2.377 0.359
V8011¯β//0001α111β//112¯0α60°/112¯0
V9011β//0001α11¯1β//112¯0α63.26°/10¯ 5 5 3¯
V10011β//0001α111¯β//112¯0α60.83°/1.377¯ 1 2.377 0.359
V11101β//0001α1¯11β//112¯0α63.26°/10¯ 5 5 3¯
V12101β//0001α111¯β//112¯0α60.83°/1.377¯ 1 2.377 0.359
表3  TC4钛合金中通过Burgers取向关系由β→α相变产生的12种变体[9,23,24]
图6  WQ和WQ-LSR试样的初始β晶粒重构及α变体取向
Grain/variantEuler angleArea fraction / %
WQWQ-LSRWQWQ-LSR
Prior β grain(319.7°, 177.7°, 95.1°)(55.2°, 85.3°, 272.0°)100.00100.00
V1(269.6°, 88.5°, 176.5°)(190.2°, 91.9°, 170.0°)5.888.70
V2(89.6°, 91.5°, 352.9°)(10.2°, 88.1°, 359.5°)5.9028.50
V3(179.6°, 91.8°, 356.2°)(100.4°, 85.2°, 352.8°)8.261.75
V4(359.6°, 88.2°, 173.2°)(280.4°, 94.8°, 176.7°)6.430.75
V5(314.4°, 42.7°, 85.0°)(237.1°, 49.8°, 82.1°)7.1025.49
V6(134.4°, 137.3°, 84.4°)(57.1°, 130.2°, 87.3°)11.742.46
V7(227.0°, 135.2°,268.0°)(140.8°, 132.8°,258.3°)7.1512.61
V8(47.0°, 44.8°, 261.4°)(320.8°, 47.2°, 271.2°)12.821.23
V9(42.3°, 134.7°, 81.5°)(330.3°, 136.8°, 91.7°)7.526.32
V10(222.3°, 45.3°, 88.0°)(150.3°, 43.2°, 77.8°)8.581.74
V11(134.8°, 47.3°, 264.5°)(53.0°, 40.3°, 267.8°)8.768.22
V12(314.8°, 132.7°, 265.0°)(233.0°, 139.7°, 261.7°)9.862.23
表4  WQ和WQ-LSR试样中原始β晶粒及其12个α变体的Euler角与面积占比
图7  WQ和WQ-LSR试样的取向差角统计
α/α boundaryRotation angle / (°)Frequency / %
WQWQ-LSR
Type 110.531.91.3
Type 26033.621.6
Type 360.836.84.6
Type 463.2647.065.1
Type 59010.67.4
表5  WQ和WQ-LSR试样变体α/α晶界长度占比统计
[1] Li Y, Zhao Y Q, Zeng W D. Application and development of aerial titanium alloys [J]. Mater. Rep., 2020, 34(suppl.1) : 280
[1] 李 毅, 赵永庆, 曾卫东. 航空钛合金的应用及发展趋势 [J]. 材料导报, 2020, 34(): 280
[2] Liu Y, Qu Z D, Wang B X. Research development and application of Ti6Al4V alloy [J]. Ordnance Mater. Sci. Eng., 2005, 28(1): 47
[2] 刘 莹, 曲周德, 王本贤. 钛合金TC4的研究开发与应用 [J]. 兵器材料科学与工程, 2005, 28(1): 47
[3] Yang Z Y, Wen F M, Sun Q, et al. Strength-ductility improvement achieved by introducing heterostructured martensite in a Ti-6Al-4V alloy [J]. Mater. Charact., 2022, 192: 112230
doi: 10.1016/j.matchar.2022.112230
[4] Pantawane M V, Sharma S, Sharma A, et al. Coarsening of martensite with multiple generations of twins in laser additively manufactured Ti6Al4V [J]. Acta Mater., 2021, 213: 116954
doi: 10.1016/j.actamat.2021.116954
[5] Karimi J, Xie M S, Wang Z, et al. Influence of substructures on the selective laser melted Ti-6Al-4V alloy as a function of laser re-melting [J]. J. Manuf. Processes, 2021, 68: 1387
doi: 10.1016/j.jmapro.2021.06.059
[6] Akhtar A. Basal slip and twinning in α-titanium single crystals [J]. Metall. Trans. A, 1975, 6: 1105
doi: 10.1007/BF02661366
[7] Ishiyama S, Hanada S, Izumi O. Orientation dependence of twinning in commercially pure titanium [J]. J. Jpn. Inst. Met. Mater., 1990, 54: 976
[8] Dai J H, Wang T T, Chai L J, et al. Characterization and correlation of microstructure and hardness of Ti-6Al-4V sheet surface-treated by pulsed laser [J]. J. Alloys Compd., 2020, 826: 154243
doi: 10.1016/j.jallcom.2020.154243
[9] Ma J K, Zhang Y S, Li J J, et al. Variant selection within one β grain in laser solid formed Ti-6Al-4V alloys [J]. Mater. Charact., 2022, 185: 111744
doi: 10.1016/j.matchar.2022.111744
[10] Vrancken B, Thijs L, Kruth J P, et al. Heat treatment of Ti6Al4V produced by Selective Laser Melting: Microstructure and mechanical properties [J]. J. Alloys Compd., 2012, 541: 177
doi: 10.1016/j.jallcom.2012.07.022
[11] Chai L J, Wu H, Zheng Z Y, et al. Microstructural characterization and hardness variation of pure Ti surface-treated by pulsed laser [J]. J. Alloys Compd., 2018, 741: 116
doi: 10.1016/j.jallcom.2018.01.113
[12] Yang J J, Yu H C, Yin J, et al. Formation and control of martensite in Ti-6Al-4V alloy produced by selective laser melting [J]. Mater. Des., 2016, 108: 308
doi: 10.1016/j.matdes.2016.06.117
[13] Wei S L, Zhu G M, Tasan C C. Slip-twinning interdependent activation across phase boundaries: An in-situ investigation of a Ti-Al-V-Fe (α + β) alloy [J]. Acta Mater., 2021, 206: 116520
doi: 10.1016/j.actamat.2020.116520
[14] Deng X G, Zhang D L, Jiao Q Y, et al. Schmid factor analysis of twinning behavior in Ti-2Al alloy [J]. Mater. Sci. Eng., 2022, A844: 143201
[15] Zhang H, Wei B Q, Ou X Q, et al. Enhancing { 10 1 ¯ 2 }   twin boundary migration capability in Ti-Al solid solution alloys with increasing Al content [J]. J. Mater. Sci. Technol., 2023, 147: 217
doi: 10.1016/j.jmst.2022.10.080
[16] Williams J C, Baggerly R G, Paton N E. Deformation behavior of HCP Ti-Al alloy single crystals [J]. Metall. Mater. Trans., 2002, 33A: 837
[17] Prakash D G L, Ding R, Moat R J, et al. Deformation twinning in Ti-6Al-4V during low strain rate deformation to moderate strains at room temperature [J]. Mater. Sci. Eng., 2010, A527: 5734
[18] Paton N E, Baggerly R G, Williams J C. Deformation and solid solution strengthening of titanium-aluminum single crystals [R]. Thousand Oaks, CA: Rockwell International Science Center, 1976
[19] Zhang G W. Effect of Al content on microstructure and properties of TC4 fabricated by laser additive manufacturing [D]. Dalian: Dalian University of Technology, 2018
[19] 张桂伟. Al含量对激光增材制造TC4组织及性能的影响 [D]. 大连: 大连理工大学, 2018
[20] Juechter V, Scharowsky T, Singer R F, et al. Processing window and evaporation phenomena for Ti-6Al-4V produced by selective electron beam melting [J]. Acta Mater., 2014, 76: 252
doi: 10.1016/j.actamat.2014.05.037
[21] Yu H, Cao S, Youssef S S, et al. Generalized stacking fault energies and critical resolved shear stresses of random α-Ti-Al alloys from first-principles calculations [J]. J. Alloy. Compd., 2021, 850: 156314
doi: 10.1016/j.jallcom.2020.156314
[22] Kishida K, Kim J G, Nagae T, et al. Experimental evaluation of critical resolved shear stress for the first-order pyramidal c  +  a slip in commercially pure Ti by micropillar compression method [J]. Acta Mater., 2020, 196: 168
doi: 10.1016/j.actamat.2020.06.043
[23] Beladi H, Chao Q, Rohrer G S. Variant selection and intervariant crystallographic planes distribution in martensite in a Ti-6Al-4V alloy [J]. Acta Mater., 2014, 80: 478
doi: 10.1016/j.actamat.2014.06.064
[24] Yang Y, Liu Y J, Chen J, et al. Crystallographic features of α variants and β phase for Ti-6Al-4V alloy fabricated by selective laser melting [J]. Mater. Sci. Eng., 2017, A707: 548
[25] Wang S C, Aindow M, Starink M J. Effect of self-accommodation on α/α boundary populations in pure titanium [J]. Acta Mater., 2003, 51: 2485
doi: 10.1016/S1359-6454(03)00035-1
[26] Jeong S G, Karthik G M, Kim E S, et al. Architectured heterogeneous alloys with selective laser melting [J]. Scr. Mater., 2022, 208: 114332
doi: 10.1016/j.scriptamat.2021.114332
[27] Simonelli M, Tse Y Y, Tuck C. On the texture formation of selective laser melted Ti-6Al-4V [J]. Metall. Mater. Trans., 2014, 45A: 2863
[28] Ahmed T, Rack H J. Phase transformations during cooling in α + β titanium alloys [J]. Mater. Sci. Eng., 1998, A243: 206
[29] Zhang Q, Xie J W, Gao Z Y, et al. A metallurgical phase transformation framework applied to SLM additive manufacturing processes [J]. Mater. Des., 2019, 166: 107618
doi: 10.1016/j.matdes.2019.107618
[30] Stephenson P L, Haghdadi N, DeMott R, et al. Effect of scanning strategy on variant selection in additively manufactured Ti-6Al-4V [J]. Addit. Manuf., 2020, 36: 101581
[31] Zhang J H, Xu D S, Wang Y Z, et al. Influences of dislocations on nucleation and micro-texture formation of α phase in Ti-6Al-4V alloy [J]. Acta Metall. Sin., 2016, 52: 905
[31] 张金虎, 徐东生, 王云志 等. 位错对Ti-6Al-4V合金α相形核及微织构形成的影响 [J]. 金属学报, 2016, 52: 905
doi: 10.11900/0412.1961.2016.00053
[32] Shi R, Wang Y. Variant selection during α precipitation in Ti-6Al-4V under the influence of local stress—A simulation study [J]. Acta Mater., 2013, 61: 6006
doi: 10.1016/j.actamat.2013.06.042
[33] Qiu D, Shi R, Zhang D, et al. Variant selection by dislocations during α precipitation in α/β titanium alloys [J]. Acta Mater., 2015, 88: 218
doi: 10.1016/j.actamat.2014.12.044
[34] Iracheta O, Bennett C J, Sun W. A sensitivity study of parameters affecting residual stress predictions in finite element modelling of the inertia friction welding process [J]. Int. J. Solids Struct., 2015, 71: 180
doi: 10.1016/j.ijsolstr.2015.06.018
[35] Payares-Asprino M C, Katsumoto H, Liu S. Effect of martensite start and finish temperature on residual stress development in structural steel welds [J]. Weld. J., 2008, 87: 279
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