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TC6鈦合金高溫準(zhǔn)靜態(tài)與室溫動(dòng)態(tài)變形條件下微結(jié)構(gòu)演化對(duì)比
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楚雄師范學(xué)院學(xué)術(shù)骨干項(xiàng)目(09YJGG02)


Comparative Studies on Microstructure Evolution of TC6 Titanium Alloy Deformed under the Condition of High Temperature Quasistatic State and High Strain-Rate
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    摘要:

    采用gleeble-1500熱模擬試驗(yàn)機(jī)及分離式霍普金森壓桿技術(shù),對(duì)TC6鈦合金試樣進(jìn)行高溫準(zhǔn)靜態(tài)(0.01 s-1)壓縮試驗(yàn)及室溫高應(yīng)變率(103 s-1)剪切試驗(yàn),通過光學(xué)顯微鏡及透射電鏡對(duì)比研究2種變形條件下材料微結(jié)構(gòu)演化特點(diǎn)。結(jié)果表明:在2種變形條件下材料微結(jié)構(gòu)演化顯著不同。在高溫準(zhǔn)靜態(tài)條件下變形時(shí),TC6鈦合金微結(jié)構(gòu)演化經(jīng)歷了4個(gè)階段:等軸狀α相變形為板條狀→板條狀α相斷裂,同時(shí)出現(xiàn)動(dòng)態(tài)再結(jié)晶晶?!鷦?dòng)態(tài)再結(jié)晶晶粒長(zhǎng)大→發(fā)生α/β相變;在高應(yīng)變率加載條件下變形時(shí),TC6鈦合金微結(jié)構(gòu)演化經(jīng)歷了3個(gè)階段:等軸狀α相變形為板條狀→位錯(cuò)的快速運(yùn)動(dòng),板條狀α相變形為更為細(xì)長(zhǎng)狹窄的長(zhǎng)條狀→長(zhǎng)條狀α相斷裂,同時(shí)出現(xiàn)少量動(dòng)態(tài)再結(jié)晶晶粒;在2種變形條件下,TC6鈦合金均發(fā)生了動(dòng)態(tài)再結(jié)晶,但高溫準(zhǔn)靜態(tài)下,動(dòng)態(tài)再結(jié)晶晶粒較多且發(fā)生長(zhǎng)大,尺寸為3~5 μm,而高應(yīng)變率加載條件下形成的動(dòng)態(tài)再結(jié)晶晶粒較少且沒有長(zhǎng)大,尺寸為0.1~0.2 μm

    Abstract:

    An high temperature quasistatic compression test (0.01 s-1) and a dynamic shearing experiment (103 s-1) on TC6 titanium alloy were performed by the gleeble-1500-type thermal simulation testing machine and a split Hopkinson bar process, respectively. Microstructure evolution of TC6 titanium alloy deformed under the condition of high temperature and high strain rate were contrastively investigated by means of optical microscope and transmission electron microscopy. Results show that the microstructure evolution of TC6 titanium alloy deformed at high temperatures is observably different from that at high strain-rate. The former includes four stages, i.e. deforming of equiaxed-type α phase to lath-shape α phase, breakdown of lath-shape α phase and simultaneous appearing and growth of dynamically recrystallized grains and phase transformation of α/β. The later goes through three stages, i.e. deforming of equiaxed-type α phase to lath-shape α phase, and then to lathy α phase due to rapid movement of dislocation, breakdown of lathy α phase and appearing of a few dynamically recrystallized grains. Under the two conditions of deforming, there is dynamically recrystallized grains occurring without exception, but there is a greater amount of dynamically recrystallized grains under the condition of high temperature and the dynamically recrystallized grains have grown up with sizes of 3-5 μm approximately. Whenas there are a few dynamically recrystallized grains that never grow up at high strain-rate with sizes of 0.1-0.2 μm approximately

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孫 坤,徐 媛,自興發(fā),劉瑞明. TC6鈦合金高溫準(zhǔn)靜態(tài)與室溫動(dòng)態(tài)變形條件下微結(jié)構(gòu)演化對(duì)比[J].稀有金屬材料與工程,2011,40(9):1561~1564.[Sun Kun, Xu Yuan, Zi Xingfa, Liu Ruiming. Comparative Studies on Microstructure Evolution of TC6 Titanium Alloy Deformed under the Condition of High Temperature Quasistatic State and High Strain-Rate[J]. Rare Metal Materials and Engineering,2011,40(9):1561~1564.]
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  • 收稿日期:2010-09-20
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