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Phase transformation behavior of a Mn containing beta-solidifying gamma-TiAl alloy during continuous cooling

机译:在连续冷却过程中含有β固化γ合金的Mn的相变行为

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The research was mainly focused on the phase transformation of Ti-42Al-5Mn (at%) alloy produced by vacuum induction melting (VIM) and vacuum arc remelting (VAR) followed by wrought process. The phase transformation kinetics of the alloy during continuous cooling under the cooling rates of 0.1 degrees C/s, 0.5 degrees C/s, 2 degrees C/s, 10 degrees C/ s, 50 degrees C/s, and 200 degrees C/s were identified by the Gleeble-3800 system, which is finally used to construct a schematic continuous cooling transformation (CCT) diagram of this alloy. The related phase composition, microstructure and property of the alloy were studied using X-ray diffraction (XRD), electron probe micro analyzer (EPMA), transmission electron microscope (TEM) and Vickers hardness (HV). It shows that six kinds of phase transformation are existed during continuous cooling from 1300 degrees C with the cooling rates of 0.1 degrees C/s, 0.5 degrees C/s, 2 degrees C/s, 10 degrees C/s, 50 degrees C/s, 200 degrees C/s and WQ, including beta -alpha(2)', beta -alpha, beta -gamma, beta -beta(o)/alpha -alpha(2), alpha(2)-alpha(2)/gamma and alpha(2)/gamma -beta(o,sec).It reveals that partial transformations would be inhibited when the cooling rate is relatively high. The martensitic structures (alpha(2)b') obtained by beta -alpha(2) were formed under the WQ condition after holding at 1300 degrees C for 5min, and it will be completely restrained below the cooling rate of WQ. For the beta -gamma, it is restrained if the cooling rates are higher than 50 degrees C/s. The alpha(2)-alpha(2)/gamma could be also suppressed when cooling with 200 degrees C/s, and the gamma lath within the supersaturated alpha(2)-grains would be formed at lower cooling rate below 50 degrees C/s. For 0.5 degrees C/s and 0.1 degrees C/s, a small amount of dotted beta(o) (beta(o,sec)) phases can be formed in the lamellar interfaces, which is proved the reaction products of alpha(2)/gamma -beta(o,sec). Furthermore, the effect of cooling rates on the microstructure, including interlamellar spacing (lambda) and gamma grains are also identified and discussed.
机译:该研究主要集中在通过真空感应熔化(Vim)产生的Ti-42-5Mn(At%)合金的相变和真空弧重熔(VAR),然后进行锻造方法。在连续冷却过程中,合金的相变动力学在连续冷却过程中,冷却速度为0.1℃/ s,0.5℃/ s,2℃/ s,10℃/ s,50℃/ s,200℃/由Gleeble-3800系统识别,最终用于构建该合金的示意性连续冷却变换(CCT)图。使用X射线衍射(XRD),电子探针微分析仪(EPMA),透射电子显微镜(TEM)和维氏硬度(HV)研究了合金的相关相组合物,微观结构和性质。它表明,在从1300摄氏度的连续冷却过程中,六种相变六种相变,冷却速率为0.1℃/ s,0.5℃/ s,2℃/ s,10摄氏度,50℃/ S,200摄氏度和WQ,包括β - &α(2)',β-&α,β - &γ,β - &β(O)/ alpha - & alpha(2) ,α(2) - &α(2)/γ和α(2)/伽马 - &β(o,sec)。揭示当冷却速率相对较高时会抑制部分变换。通过β - &α(2)获得的马氏体结构(α(2)&')在持有1300℃的WQ条件下形成5min,并且将完全限制在冷却速度以下WQ。对于β - &伽玛,如果冷却速率高于50度C / s,则会受到限制。当用200℃/ s的冷却时,α(2) - &gγ也可以抑制α(2)/γ,并且在超过50度以下的冷却速率下,将γ内的γα(2)-Grains内的γ板块形成CS。对于0.5℃/ s和0.1℃/ s,可以在层状界面中形成少量点β(o)(β(o,o,sec))相,这被证明了α(2)的反应产物/伽玛 - & beta(o,sec)。此外,还鉴定并讨论了冷却速率对微观结构的影响,包括层间距(Lambda)和γ晶粒。

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