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Anomalous resistivity change in β brass by annealing below 523K

机译:在523K以下退火导致β黄铜的电阻率异常变化

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Two sorts ofβ single phase and anα + β two phase Cu- Zu alloys were annealed below 523K.Detailed investigation on anomalous resistivity increase has cleared following facts. The resistivityincrease is occured by annealing below 473K, even under coexistence ofα phase. During holding atroom temperature, the once increased resistivity gradually decreases to nearly same value beforeannealing. Therefore, the increase in resistivity is reversible and amount of increase is determined byannealing temperature. The amount of resistivity increase becomes larger with elevated annealingtemperature up to 423K, in opposite sence to G. P. zone formation in aluminium alloys. From theseobservations, this increase can not be interpreted by any precursor of martensitic transformation, andit should be caused by increase in concentration of "wrong atom", as previous predictions. However,the reason why this phenomenon occurs is the remaining problem. As a subproduct, it is confirmedthat the resistivity ofβ phase shows negative dependence on Zn concentration or, the resistivitydecreases with increasing Zn content, represented byρ{sub}(β77)Ωm = 97.26 -1.765C{sup}(zn)/at%.
机译:在523K以下对两种β单相和α+β两相Cu-Zu合金进行了退火。对电阻率反常增加的详细研究已经消除了以下事实。即使在α相共存的情况下,通过在473K以下进行退火,电阻率也会增加。在保持室温的过程中,曾经增加的电阻率在退火之前逐渐降低到几乎相同的值。因此,电阻率的增加是可逆的,并且增加的量由退火温度确定。与升高的退火温度直至423K相比,电阻率的增加量变大,这与铝合金中的G. P.区形成相反。从这些观察中,这种增加不能由马氏体相变的任何前体来解释,而应该由先前所预测的“错误原子”的浓度增加引起。然而,这种现象发生的原因仍然是问题。作为副产品,可以确定β相的电阻率与Zn浓度呈负相关关系,或者电阻率随Zn含量的增加而降低,由ρ{sub}(β77)Ωm= 97.26 -1.765C {sup}(zn)/ at%表示。 。

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