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GH625合金的動(dòng)態(tài)再結(jié)晶行為研究
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Dynamic Recrystallization Behavior of GH625 Superalloy during Hot Deformation
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    摘要:

    采用Gleeble-3800熱模擬試驗(yàn)機(jī)研究了GH625合金在變形溫度為950~1150 ℃,應(yīng)變速率為0.001~5 s-1條件下的熱變形特性,并用OM和TEM分析了變形條件對(duì)微觀結(jié)構(gòu)的影響。結(jié)果表明:當(dāng)應(yīng)變量很小時(shí),該合金沒(méi)有發(fā)生再結(jié)晶,直到應(yīng)變量達(dá)到0.1時(shí)才開(kāi)始有再結(jié)晶晶粒析出。隨著變形溫度的升高,再結(jié)晶晶粒尺寸增大,位錯(cuò)密度降低;當(dāng)溫度較低時(shí)顯微結(jié)構(gòu)中可以觀察到孿晶。當(dāng)變形溫度一定時(shí),隨應(yīng)變速率的增大,再結(jié)晶的形核率增大且晶粒變小,位錯(cuò)密度變大;而當(dāng)應(yīng)變速率較低時(shí),再結(jié)晶進(jìn)行得比較充分,晶粒尺寸較大。根據(jù)實(shí)測(cè)的應(yīng)力-應(yīng)變曲線(xiàn),獲得了該合金發(fā)生動(dòng)態(tài)再結(jié)晶的臨界應(yīng)變?chǔ)與和峰值應(yīng)變?chǔ)舙與Z參數(shù)之間的關(guān)系:εc=2.0×10-3·Z0.123 85,lnεp= –6.022 85+0.123 85lnZ。此外,還采用定量金相法計(jì)算出了合金的動(dòng)態(tài)再結(jié)晶體積分?jǐn)?shù),并建立了該合金動(dòng)態(tài)再結(jié)晶的動(dòng)力學(xué)模型:Xd=1–exp[–0.5634(ε/εp–0.79)1.313]。

    Abstract:

    The deformation behavior of GH625 superalloy was studied by the isothermal compression test in the temperature range of 950~ 1150 °C and the strain rate range of 0.001~5 s-1 and the effect of deformation condition on the microstructure was also investigated by OM and TEM. Results show that the dynamic recrystallization do not occur as the strain is little while the recrystallized grains appear when ε=0.1. As the deformation temperature increases, the recrystallized grain size increases and the dislocation density decreases; when the deformation temperature is low, some twins are observed in the matrix. As the strain rate increases, the nucleation rate increases and the grain size decreases, while the dislocation density increases at a constant deformation temperature; while at the low strain rate, the degree of recrystallization is high, which lead to the increase of grain size. According to stress-strain curves, the peak strain, the critical strain and the steady strain are obtained, and the relationship between the logarithmic values of the critical strain for DRX initiation () and the logarithmic value of the Zener-Hollomon parameter (lnZ) could be established as follows: lnεp= –6.022 85+0.123 85lnZ, εc=2.0×10-3·Z0.123 85. On the basis of quantitative microstructure analysis, the recrystallized volume fraction is also established as Xd=1–exp[–0.5634(ε/εp–0.79)1.313].

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周海濤,劉志超,溫盛發(fā),李偉東,周 嘯. GH625合金的動(dòng)態(tài)再結(jié)晶行為研究[J].稀有金屬材料與工程,2012,41(11):1917~1922.[Zhou Haitao, Liu Zhichao, Wen Shengfa, Li Weidong, Zhou Xiao. Dynamic Recrystallization Behavior of GH625 Superalloy during Hot Deformation[J]. Rare Metal Materials and Engineering,2012,41(11):1917~1922.]
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  • 收稿日期:2011-11-24
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