Low-Cycle Fatigue Life and Plasticity Mechanisms of a Fe−15Mn−10Cr−8Ni−4Si Seismic Damping Alloy Under Cyclic Loading at Various Temperatures

T. Sawaguchi, I. Nikulin, K. Ogawa, S. Takamori, Fumiyoshi Yoshinaka, Yuya Chiba, H. Otsuka, Yasuhiko Inoue, A. Kushibe
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引用次数: 10

Abstract

A recently developed Fe−15Mn−10Cr−8Ni−4Si (FMS) seismic damping alloy has a superior fatigue life at room temperature due to reversible dislocation motion associated with the γ → e martensitic transformation. The effect of temperature on the low-cycle fatigue life (N f) and the associated plasticity mechanisms of the FMS alloy were evaluated between 253 and 393 K. The longest (N f of 15,644 was obtained at 313 K. The (N f was dependent on the plasticity mechanisms, which were subdivided into three temperature regions with respect to the upper temperature limits for stress-assisted and strain-induced martensitic transformation (Msσ and Mdσ, respectively). At temperatures below Msσ, the Nf exceeded 5,000 cycles, where e-martensite was dominant and a long period stacking ordered structure was formed. The longest Nf values of over 10,000 cycles were obtained in the dual γ/e-phase formed between Mdσ and Mdσ, while Nf decreased rapidly as the deformation temperature increased beyond Mdσ. The effect of temperature on the N f of the FMS alloy was comparable to that of Fe–28Mn–6Si–5Cr shape memory alloy, and to the chemical composition dependence of N f of Fe–30Mn–(6 – x)Si–x Al (x= 0-6) transformation- and twinning-induced plasticity (TRIP/TWIP) steels. A new set of thermodynamic parameters was established to calculate the Gibbs free energy difference between the phases (ΔGγ→e) and the stacking fault energy of austenite (ΓSFE). The superior N f was associated with the cyclic strain-induced martensitic transformation when ΔGγ→e was between –50 and 100 Jmol-1, while reversible martensitic transformation relied on a ΔGγ→e of ~0 Jmol-1.
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Fe - 15Mn - 10Cr - 8Ni - 4Si抗震阻尼合金在不同温度下的低周疲劳寿命及塑性机理
最近研制的Fe−15Mn−10Cr−8Ni−4Si (FMS)地震阻尼合金,由于与γ→e马氏体相变相关的可逆位错运动,在室温下具有优异的疲劳寿命。在253 ~ 393 K范围内,研究了温度对FMS合金低周疲劳寿命的影响及其塑性机制。在313 K时获得了最长的nf(15,644)。(N f)与塑性机制有关,根据应力诱导马氏体相变和应变诱导马氏体相变的温度上限(分别为Msσ和Mdσ),将塑性机制划分为3个温度区域。当温度低于Msσ时,Nf超过5000次循环,以e-马氏体为主,形成长周期的有序堆积结构。在Mdσ和Mdσ之间形成的双γ/e相中,Nf值超过10,000次循环的时间最长,而当变形温度超过Mdσ时,Nf值迅速下降。温度对FMS合金的N - f的影响与Fe-28Mn-6Si-5Cr形状记忆合金相当,与Fe-30Mn - (6 - x) Si-x Al (x= 0-6)相变和孪晶诱导塑性(TRIP/TWIP)钢的N - f的化学成分依赖性相当。建立了一套新的热力学参数来计算相之间的吉布斯自由能差(ΔGγ→e)和奥氏体的层错能(ΓSFE)。当ΔGγ→e为-50 ~ 100 Jmol-1时,较高的N - f与循环马氏体转变有关,而可逆马氏体转变依赖于ΔGγ→e为~0 Jmol-1。
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