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首页> 外文期刊>Acta Materialia >PHASE DECOMPOSITION OF THE y PHASE IN A Mn-30 at. Cu ALLOY DURING AGING
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PHASE DECOMPOSITION OF THE y PHASE IN A Mn-30 at. Cu ALLOY DURING AGING

机译:Mn-30 at。处的y相的相分解老化过程中的铜合金

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The phase decomposition process of γ phase in a Mn-30 at. Cu alloy, when aged at 723 K from 2 to 50 h, is investigated with electrical resistivity and magnetic susceptibility measurement. In con- junction with the antiferro-magnetic transition of the Mn-rich regions during cooling to room temperature from the aging temperature, the temperature coefficient of electrical resistivity shows a continuous increase in a certain temperature range. The temperature where the coefficient has the maximum increasing rate is defined as the T_N temperature of the Mn-rich regions. It was found that the T_N temperature was 20-30 K higher than the concomitant f.c.c.-f.c.t. transformation temperature T_t determined with the minima of Young's modulus in the aged samples. The increment of temperature coefficient of electrical resistivity involved in the magnetic transition is used to estimate the changes of volume fraction for Mn-rich regions vs aging time. At the same time, the paramagnetic feature above the spin-freezing transition temperature for quenched Cu-rich alloys is summarized, and the Mn concentration in Cu-rich regions of aged samples is calculated. It should be noted that Mn and Cu-rich regions had already formed in the 2 h-aged Mn-30 at. Cu sample, and longer aging further enriched Mn or Cu, while the volume fraction of Mn-rich regions decreased slightly with aging time. Electrical resistivity measurement sensitive to Mn-rich regions and the magnetic susceptibility measurement for Cu-rich regions have shown the compositional heterogen- eity in decomposed phases. TEM observation
机译:Mn-30 at中γ相的相分解过程。研究了在723 K下2至50 h时效的Cu合金的电阻率和磁化率测量。在从时效温度冷却至室温的过程中,富锰区的反铁磁跃迁结合在一起,电阻率温度系数在一定温度范围内显示出连续增加的趋势。将系数具有最大增加率的温度定义为富锰区域的T_N温度。发现T_N温度比伴随的f.c.c.-f.c.t高20-30K。时效温度T_t由杨氏模量的最小值确定。磁跃迁中涉及的电阻率温度系数的增量用于估算富锰区域的体积分数随老化时间的变化。同时,总结了淬火富铜合金自旋转变温度以上的顺磁特征,并计算了时效样品富铜区的锰浓度。应当指出,在2 h时效的Mn-30 at中已经形成了富锰和富铜区域。铜样品和更长的时效会进一步富集锰或铜,而富锰区的体积分数会随着时效时间而略有下降。对富锰区域敏感的电阻率测量和富铜区域的磁化率测量显示了分解相中的成分异质性。 TEM观察

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