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

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中國有色金屬學(xué)報

ZHONGGUO YOUSEJINSHU XUEBAO

第21卷    第9期    總第150期    2011年9月

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文章編號:1004-0609(2011)09-2151-06
Cu66Ti34非晶合金凝固過程的分子動力學(xué)模擬
邱克強(qiáng), 厲 虹, 孫 晶, 尤俊華, 任英磊, 李慶豐

(沈陽工業(yè)大學(xué) 材料科學(xué)與工程學(xué)院,沈陽 110870)

摘 要: 采用分子動力學(xué)模擬了二元合金Cu66Ti34的凝固過程。原子間作用采用GEAM勢,利用偶關(guān)聯(lián)函數(shù),均方位移(MSD)等分析方法,研究Cu66Ti34合金在4×1013 K/s冷卻速度下的玻璃化轉(zhuǎn)變溫度、原子的擴(kuò)散行為。結(jié)果表明,通過偶分布函數(shù)第一谷的最小值與第一峰最大值之比獲得的玻璃轉(zhuǎn)變溫度為600 K,與相近成分Cu50Ti50的實驗值接近;在800 K時,Cu和Ti的MSD最大值均小于1×10−2 nm2,合金熔體很粘稠;在600 K時,曲線的斜率降低,在動力學(xué)上合金熔體已經(jīng)凝固。定壓比熱容與溫度成二次分布關(guān)系,存在一個峰值溫度為892 K的熱力學(xué)玻璃轉(zhuǎn)變溫度,證明了用動力學(xué)方法和用熱力學(xué)方法獲得的玻璃轉(zhuǎn)變溫度之間的差異。

 

關(guān)鍵字: Cu66Ti34合金;分子動力學(xué)模擬;玻璃轉(zhuǎn)變溫度;均方位移;熱力學(xué)分析

Solidification process of Cu66Ti34 amorphous alloy
 simulated by molecular dynamics
QIU Ke-qiang, LI Hong, SUN Jing, YOU Jun-hua, REN Ying-lei, LI Qing-feng

School of Materials Science and Engineering, Shenyang University of Technology, Shenyang 110870, China

Abstract:The solidification process of Cu66Ti34 binary alloy was studied by molecular dynamics simulation. The general embedded atomic (GEAM) potential was selected as many-body interaction. The analytical methods, such as pair correction function (PCF) and mean square displacement (MSD), were employed to calculate the glass transition temperature (Tg) and the diffusion behaviors of, atoms at cooling rate of 4×1013 K/s. The results show that the glass transition temperature obtained from inflection point of the curve is 600 K, which is the ratio of minimum to maximum of the first peak of PCF for Cu66Ti34 alloy, and is comparable to that of Cu50Ti50 alloy. The maximum of MSD is lower than 1×10−2 nm2 when the temperature is 800 K, showing that the melt is very sticky. However, when the temperature reaches 600 K, the slope of the curve becomes smaller, showing that the melt is frozen dynamically, which shows that the glass transition temperature varies possibly in certain range due to dynamical factor. Simultaneously, the calculated specific heat capacity (cp) at constant pressure shows that it distributes in secondary order vs temperature. The peak temperature or the glass transition temperature is 892 K, which shows the difference between the glass transition temperatures obtained by dynamics and thermodynamics, respectively.

 

Key words: Cu66Ti34 alloy; molecular dynamic simulation; glass transition temperature; mean square displacement; thermodynamical analysis

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

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

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