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/鋁爆炸焊接界面擴(kuò)散行為分子動(dòng)力學(xué)模擬
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1.太原科技大學(xué) 材料科學(xué)與工程學(xué)院,山西 太原 030024;2.山西師范大學(xué)現(xiàn)代文理學(xué)院 轉(zhuǎn)設(shè)籌備處,山西 臨汾 041000

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基金項(xiàng)目:

國(guó)家重點(diǎn)研發(fā)計(jì)劃(2018YFA0707305);山西省科技重大專項(xiàng)(202101120401008);山西省重點(diǎn)研發(fā)計(jì)劃(202102050201001);臨汾市重點(diǎn)研發(fā)計(jì)劃(2202);山西省高等學(xué)??萍紕?chuàng)新項(xiàng)目(2022L628)


Molecular Dynamics Simulation of Diffusion Behavior of Ti/Al Explosive Welding Interface
Author:
Affiliation:

1.School of Materials Science and Engineering, Taiyuan University of Science and Technology, Taiyuan 030024, China;2.Preparatory Department, Modern College of Humanities and Sciences, Shanxi Normal University, Linfen 041000, China

Fund Project:

National Key Research and Development Program (2018YFA0707305); Major Science and Technology Projects of Shanxi Province (202101120401008); Key R&D Program of Shanxi Province (202102050201001); Linfen Key Research and Development Plan (2202); Science and Technology Innovation Project of Colleges and Universities in Shanxi Province (2022L628)

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    摘要:

    為揭示鈦/鋁爆炸焊接界面原子的擴(kuò)散行為,采用分子動(dòng)力學(xué)模擬從原子尺度分析了鈦/鋁爆炸焊接界面原子的微觀擴(kuò)散機(jī)理。利用Materials Studio建立了鈦/鋁爆炸焊接焊點(diǎn)處的分子動(dòng)力學(xué)模型,結(jié)合爆炸焊接的物理過(guò)程,將爆炸焊接過(guò)程分為加載和卸載2個(gè)階段,通過(guò)LAMMPS程序計(jì)算了爆炸焊接鈦、鋁原子的均方位移、徑向分布函數(shù)、擴(kuò)散層厚度等,利用OVITO軟件再現(xiàn)了不同階段界面原子的擴(kuò)散行為。在爆炸焊接加載階段,鈦、鋁原子不發(fā)生擴(kuò)散,只在平衡位置做振動(dòng),鋁原子振動(dòng)要比鈦原子振動(dòng)強(qiáng)。爆炸焊接卸載開始時(shí),鈦、鋁原子發(fā)生互擴(kuò)散。鈦/鈦原子鍵能高,不易破壞,鋁/鋁原子鍵能低,容易破壞產(chǎn)生空位、間隙等缺陷,有利于鈦原子深入擴(kuò)散到鋁晶格內(nèi)部,但鋁原子難以進(jìn)入鈦的晶格內(nèi)部。采用掃描電鏡和EDS能譜表征了鈦/鋁爆炸焊接復(fù)合材料界面元素分布,與模擬結(jié)果有很好的一致性。

    Abstract:

    In order to reveal the diffusion behavior of Ti/Al interface, the molecular dynamics simulation was applied to study the microscopic diffusion mechanisms of Ti/Al explosive welding interface at the atomic scale. Molecular dynamics model of Ti/Al explosive welding spot was established by Materials Studio (MS). According to the physical process of explosive welding, the simulation of the collision was divided into two stages: the loading stage and the unloading stage. The mean square displacement (MSD), radial distribution function (RDF), and diffusion layer thickness were calculated by LAMMPS, and the diffusion behavior of interfacial atoms at different stages was reproduced by OVITO. Results show that in the loading stage of explosive welding, Ti and Al atoms do not diffuse but only vibrate at the equilibrium position, and the vibration of Al atoms is stronger than that of Ti atoms. The atomic diffusion only occurs in the unloading stage of the explosive welding process. The Ti-Ti bonding energy is too high to break. The Al-Al bonding energy is low, so it is easy to be damaged, resulting in vacancies, gaps and other defects, which promotes the deep diffusion of Ti atoms into the Al substrate lattice while hindering Al atoms from entering the Ti substrate lattice. The simulation result is basically in accordance with EDS experimental result.

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李巖,劉琪,李聚才,劉翠榮,吳志生.鈦/鋁爆炸焊接界面擴(kuò)散行為分子動(dòng)力學(xué)模擬[J].稀有金屬材料與工程,2023,52(6):2017~2023.[Li Yan, Liu Qi, Li Jucai, Liu Cuirong, Wu Zhisheng. Molecular Dynamics Simulation of Diffusion Behavior of Ti/Al Explosive Welding Interface[J]. Rare Metal Materials and Engineering,2023,52(6):2017~2023.]
DOI:10.12442/j. issn.1002-185X.20221003

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  • 收稿日期:2022-12-31
  • 最后修改日期:2023-05-28
  • 錄用日期:2023-02-14
  • 在線發(fā)布日期: 2023-07-03
  • 出版日期: 2023-06-30