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Nb10Ti61Co29包共晶合金定向凝固組織演化及其凝固路徑模擬計(jì)算
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桂林電子科技大學(xué)

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TG

基金項(xiàng)目:

國家自然科學(xué)(51761009和51701048)、廣西自然科學(xué)(2020GXNSFAA159163)、桂林電子科技大學(xué)研究生教育創(chuàng)新計(jì)劃項(xiàng)目(2019YCXS109)和廣西信息材料重點(diǎn)實(shí)驗(yàn)室(191021-Z)資助


Microstructure evolution and simulation of solidification path in Nb10Ti61Co29 quasi-peritectic alloy
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School of Materials Science and Engineering,Guilin University of Electronic Technology

Fund Project:

The National Natural Science Foundation of China (51761009 and 51701048),The Natural Science Foundation of Guang Xi(2020GXNSFAA159163),the Guangxi Key Laboratory of Information Laboratory (191021-Z).

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    摘要:

    包共晶反應(yīng),兼具共晶和包晶反應(yīng)的雙重特性,存在于眾多三元合金體系中。然而,人們對其凝固特點(diǎn)了解較少,其凝固機(jī)制到目前為止尚不明確?;诖?本文選擇包共晶點(diǎn)附近的Nb10Ti61Co29合金為研究對象,利用Bridgman定向凝固技術(shù)對其開展了一系列定向凝固實(shí)驗(yàn)(v=1, 3, 5, 15, 30, 70 μm/s),然后利用XRD,SEM和EDS等分析了不同生長速率下的凝固組織,闡明定向凝固組織演化規(guī)律,最終得出相應(yīng)的凝固機(jī)理。研究結(jié)果表明,不同生長速率下合金的凝固組織均包含初始過渡區(qū)、穩(wěn)態(tài)生長區(qū)以及淬火區(qū)。隨著生長速率逐漸增大,初始過渡區(qū)上初始生長界面輪廓越來越清晰,并逐漸趨于平直狀態(tài),伴隨上述變化,穩(wěn)態(tài)生長區(qū)與初始過渡區(qū)關(guān)聯(lián)性逐漸變?。黄浯?隨著生長速率逐漸增大,合金淬火界面依次經(jīng)歷平界面向胞狀晶再到樹枝晶的轉(zhuǎn)變,其中,淬火界面在生長速率為1 μm/s時呈平直狀態(tài),在生長速率為3和5 μm/s時,淬火界面大致呈胞狀,當(dāng)生長速率進(jìn)一步增大時淬火界面呈現(xiàn)典型的枝晶生長;最后,利用CALPHAD方法計(jì)算得出了該合金在平衡凝固過程中會依次發(fā)生如下四個凝固反應(yīng):(a) L→α-Nb;(b) 二元共晶反應(yīng)L→α-Nb + TiCo;(c) 三元包共晶反應(yīng)L + TiCo→α-Nb + Ti2Co 和 (d) 二元共晶反應(yīng)L→α-Nb + Ti2Co。

    Abstract:

    The quasi-peritectic reaction, which has dual characteristics of eutectic and peritectic reaction, exists in many ternary alloy systems. However, its solidification characteristics and its solidification mechanism is still unclear so far. To address this question, the Nb10Ti61Co29 alloy near the quasi-peritectic point was selected as the research object in this paper, and a series of directional solidification experiments with different growth rates (ν=1, 3, 5, 15, 30, 70 μm/s) were carried out using Bridgman directional solidification technique. Then the solidification structure at each growth rate was analyzed by XRD, SEM and EDS, and the microstructure evolution law of these directionally solidified samples was clarified. The results show that, the solidification structure of this alloy at different growth rates includes initial transition zone, steady-state growth zone and quenching zone. As the growth rate increases, the profile of the initial growth interface in the initial transition zone becomes more and more clear. With these changes, the relationship between the steady-state growth region and the initial transition region becomes smaller. Moreover, the quenching interfaces go through the transition from flat-bound to cell-oriented to dendrite in turn with the increase of the growth rate. In especial, the quenching interface is flat when the growth rate is 1 μm/s, whereas the quenching interface is roughly cellular when the growth rates are 3 and/or 5 μm/s. Lastly, the following four solidification reactions will occur successively in the process of equilibrium solidification, which was calculated by CALPHAD method, (a) L→α-Nb; (b) binary eutectic reaction L→α-Nb + TiCo;α-Nb TiCo; (c) ternary quasiperitecticcoated reaction L+TiCo→α-Nb +Ti2Co and (d) binary eutectic reaction L→α-Nb + Ti2Co.

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狄翀博,閆二虎,陳運(yùn)燦,王金華,劉威,王豪,孫立賢. Nb10Ti61Co29包共晶合金定向凝固組織演化及其凝固路徑模擬計(jì)算[J].稀有金屬材料與工程,2021,50(9):3194~3202.[DI Chongbo, YAN Erhu, CHEN Yuncan, WANG Jinhua, LIU Wei, WANG Hao, SUN Lixian. Microstructure evolution and simulation of solidification path in Nb10Ti61Co29 quasi-peritectic alloy[J]. Rare Metal Materials and Engineering,2021,50(9):3194~3202.]
DOI:10.12442/j. issn.1002-185X.20200704

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  • 收稿日期:2020-09-14
  • 最后修改日期:2020-12-07
  • 錄用日期:2020-12-22
  • 在線發(fā)布日期: 2021-09-27
  • 出版日期: 2021-09-24