(Shockley)位錯(cuò)長(zhǎng)度的顯著降低,以及FCC晶體結(jié)構(gòu)的原子數(shù)目向Other和HCP晶體結(jié)構(gòu)的最大轉(zhuǎn)變速率,導(dǎo)致θ=90°時(shí)單晶鎳的損傷演化速率最快且損傷程度最劇烈。值得注意的是,當(dāng)θ=90°時(shí)單晶鎳中孔洞最易聚集這是由于該條件下孔洞表面受到更大的拉應(yīng)力作用所導(dǎo)致。通過(guò)該工作,旨在揭示金屬材料在高應(yīng)變率下的孔洞聚集行為及機(jī)理,并對(duì)揭示其軟化行為和斷裂機(jī)理提供了理論指導(dǎo)。"/>

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含孔洞缺陷的單晶鎳?yán)煨袨椋嚎锥瓷L(zhǎng)和聚集機(jī)理
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重慶理工大學(xué)機(jī)械工程學(xué)院

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TG 146

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國(guó)家自然科學(xué)基金委員會(huì)與中國(guó)工程物理研究院聯(lián)合(批準(zhǔn)號(hào):U1530140)、重慶市教育委員會(huì)科學(xué)技術(shù)研究(批準(zhǔn)號(hào):KJQN202001126)資助項(xiàng)目.


Tensile behavior of single-crystal nickel containing void defects: void growth and coalescence mechanisms
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    摘要:

    利用分子動(dòng)力學(xué)模擬研究了孔洞中心形成平面與加載方向的夾角(θ)對(duì)單晶鎳在單軸拉伸下孔洞生長(zhǎng)和聚集行為的影響及機(jī)理。結(jié)果表明:?jiǎn)尉ф嚨那?yīng)力和平均流動(dòng)應(yīng)力隨著夾角θ的增加而下降,應(yīng)力下降速率隨著夾角θ的增加而加快。當(dāng)夾角θ=90°時(shí)(加載方向垂直于孔洞中心平面時(shí)),單晶鎳中孔洞獨(dú)立生長(zhǎng)時(shí)間最短且孔洞之間最先發(fā)生聚集,導(dǎo)致其最易進(jìn)入軟化階段,這是由于夾角θ=90°時(shí),單晶鎳中最快的孔洞體積分?jǐn)?shù)增長(zhǎng)速率和損傷演化速率所導(dǎo)致。當(dāng)夾角θ=90°時(shí),單晶鎳中1/6<112>(Shockley)位錯(cuò)長(zhǎng)度的顯著降低,以及FCC晶體結(jié)構(gòu)的原子數(shù)目向Other和HCP晶體結(jié)構(gòu)的最大轉(zhuǎn)變速率,導(dǎo)致θ=90°時(shí)單晶鎳的損傷演化速率最快且損傷程度最劇烈。值得注意的是,當(dāng)θ=90°時(shí)單晶鎳中孔洞最易聚集這是由于該條件下孔洞表面受到更大的拉應(yīng)力作用所導(dǎo)致。通過(guò)該工作,旨在揭示金屬材料在高應(yīng)變率下的孔洞聚集行為及機(jī)理,并對(duì)揭示其軟化行為和斷裂機(jī)理提供了理論指導(dǎo)。

    Abstract:

    Molecular dynamics simulations were used to investigate the effect and mechanism of the angle (θ) between the plane of void center formation and the loading direction on void growth and coalescence behavior in single-crystal nickel under uniaxial tension. The results show that the yield stress and average flow stress of single-crystal nickel decrease with increasing θ, and the rate of stress decrease accelerates with increasing θ. When θ=90° (loading direction perpendicular to the plane of void center), the independent growth time of voids in single-crystal nickel is the shortest and void coalescence occurs first, leading to the most easily entering the softening stage. This is due to the fastest growth rate of void volume fraction and damage evolution rate in single-crystal nickel when θ=90°. When θ=90°, the significant reduction of 1/6<112> (Shockley) dislocation length and the maximum transformation rate of atomic number from FCC crystal structure to Other and HCP crystal structures in single-crystal nickel lead to the fastest damage evolution rate and the most severe damage level when θ=90°. It is worth noting that voids in single-crystal nickel are most likely to coalesce when θ=90°, due to the larger tensile stress on the void surface under this condition. Through this work, the aim is to reveal the void coalescence behavior and mechanism of metallic materials under high strain rates, and to provide theoretical guidance for understanding their softening behavior and fracture mechanism.

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宋鹍,黃霞.含孔洞缺陷的單晶鎳?yán)煨袨椋嚎锥瓷L(zhǎng)和聚集機(jī)理[J].稀有金屬材料與工程,2023,52(11):3767~3777.[songkun, huangxia. Tensile behavior of single-crystal nickel containing void defects: void growth and coalescence mechanisms[J]. Rare Metal Materials and Engineering,2023,52(11):3767~3777.]
DOI:10.12442/j. issn.1002-185X.20230187

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  • 收稿日期:2023-04-06
  • 最后修改日期:2023-06-07
  • 錄用日期:2023-06-07
  • 在線發(fā)布日期: 2023-11-27
  • 出版日期: 2023-11-22