Transactions of Nonferrous Metals Society of China The Chinese Journal of Nonferrous Metals

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中國(guó)有色金屬學(xué)報(bào)

ZHONGGUO YOUSEJINSHU XUEBAO

第24卷    第8期    總第185期    2014年8月

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文章編號(hào):1004-0609(2014)08-2073-10
晶界位錯(cuò)發(fā)射與湮沒(méi)過(guò)程的晶體相場(chǎng)模擬
高英俊1, 2,盧成健1, 3,羅志榮1, 3,林 葵1, 2,黃創(chuàng)高1, 2

(1. 廣西大學(xué) 物理科學(xué)與工程技術(shù)學(xué)院,南寧 530004;
2. 廣西大學(xué) 廣西有色金屬及特色材料加工重點(diǎn)實(shí)驗(yàn)室,南寧 530004;
3. 玉林師范學(xué)院 物理科學(xué)與工程技術(shù)學(xué)院,玉林 537000
)

摘 要: 采用晶體相場(chǎng)模型模擬位向差為7.70°的對(duì)稱(chēng)傾側(cè)晶界位錯(cuò)在外加應(yīng)力作用下的運(yùn)動(dòng)形式和演化過(guò)程;計(jì)算位錯(cuò)分離的激活能,并從能量變化角度分析位錯(cuò)運(yùn)動(dòng)過(guò)程中發(fā)生的分解、湮沒(méi)和合并機(jī)制;分析該對(duì)稱(chēng)傾側(cè)晶界在外力作用下晶界湮沒(méi)過(guò)程不同特征階段的差異。結(jié)果表明,晶界的湮沒(méi)存在不同的特征階段,主要階段如下:位錯(cuò)的攀移,位錯(cuò)的分解與滑移,位錯(cuò)湮沒(méi);位錯(cuò)的再攀移與位錯(cuò)再分解、再湮沒(méi),或者出現(xiàn)了若干短暫的新階段,如滑移位錯(cuò)與晶界上其他位錯(cuò)發(fā)生合并而被晶界吸收,或者滑移位錯(cuò)與另一滑移位錯(cuò)在晶內(nèi)發(fā)生合并形成新位錯(cuò)組,或者滑移位錯(cuò)與另一滑移位錯(cuò)發(fā)生湮沒(méi)消失。晶界上全位錯(cuò)的分解實(shí)質(zhì)是產(chǎn)生了一對(duì)新的符號(hào)相反的柏氏矢量;分位錯(cuò)在晶界上的湮沒(méi)或合并實(shí)質(zhì)是分位錯(cuò)與晶界上的全位錯(cuò)形成的一對(duì)符號(hào)相反的柏氏矢量發(fā)生抵消;分位錯(cuò)與分位錯(cuò)在晶粒內(nèi)部的湮沒(méi)消失,其實(shí)質(zhì)是2個(gè)分位錯(cuò)之間的2對(duì)符號(hào)完全相反的位錯(cuò)柏氏矢量相互抵消。

 

關(guān)鍵字: 晶界;位錯(cuò);湮沒(méi);分解;晶體相場(chǎng)模型

Phase field crystal simulation of dislocation emission and annihilation at grain boundary
GAO Ying-jun1, 2, LU Cheng-jian1, 3, LUO Zhi-rong1, 3, LIN Kui1, 2, HUANG Chuang-gao1, 2

1. College of Physics Science and Engineering, Guangxi University, Nanning 530004, China;
2. Guangxi Key Laboratory for Non-ferrous Metal and Featured Materials, Guangxi University, Nanning 530004, China;
3. Institute of Physics Science and Engineering Technology, Yulin Normal University, Yulin 537000, China

Abstract:The movement and evolution of the dislocation for a low-angle grain boundary (GB) with orientation of 7.70° under stress were simulated by using the phase-field crystal model. The dislocation reaction of separation, annihilation and mergence and these mechanisms were analyzed from the energy point of view, and the activation energy of dislocation separation was calculated. The difference of feature stages for the annihilation process of dislocation under stress was shown through comparing two grain boundaries with different misorientations. The results show the obvious difference of typical stages of the annihilation process of GB. The main stages of GB annihilation include the dislocation climb, dislocation separation and dislocation slide, dislocation annihilation; again the dislocation climb and dislocation separation, dislocation annihilation, or instead of the dislocation climb, some new stages presented during the GB annihilation. For example, the sliding dislocation is merged by the dislocation inside the GB or absorbed by GB, or one sliding dislocation reacts with another sliding dislocation in the grain to merge into a new dislocation pairs, or the sliding dislocation reacts with another dislocation to present annihilation and disappear. The essence of dissociation of the full dislocation is that the new dislocation pairs with opposite Burgers vector are created, while that of annihilation or merge of dislocations is that the pair opposite Burgers vectors between the partial dislocation and the full dislocation on the grain boundary bring about to counteract. The annihilation of two dislocation pairs in the grain is produced by perfect counteracting of the two-opposite-pair Burgers vectors of these two dislocation pairs.

 

Key words: grain boundary; dislocation; annihilation; separation; phase-field crystal

ISSN 1004-0609
CN 43-1238/TG
CODEN: ZYJXFK

ISSN 1003-6326
CN 43-1239/TG
CODEN: TNMCEW

主管:中國(guó)科學(xué)技術(shù)協(xié)會(huì) 主辦:中國(guó)有色金屬學(xué)會(huì) 承辦:中南大學(xué)
湘ICP備09001153號(hào) 版權(quán)所有:《中國(guó)有色金屬學(xué)報(bào)》編輯部
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