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银合金应力-应变曲线的模式分析。(第1部分)银-铜合金的应力-应变曲线(作者译)

[A pattern analysis of stress-strain curves for Ag alloys. (Part 1) On stress-strain curves for Ag-Cu alloys (author's transl)].

作者信息

Yoshida J

出版信息

Shika Rikogaku Zasshi. 1976 Sep;17(39):211-21.

PMID:1069037
Abstract

Mechanical properties of the dental metals have been estimated from the value of tensile strength, yield point, elastic limit, elongation and so on. But when applying these values to practical dental problems, they are often find to be not available enough. And recently the electoronic computer has been developed and widyly used in various fields, so the author tried to analyze true stress-true strain curves for alloys as pattern by the computer. The flow curves in the region of uniform plastic deformation was expressed by the Hollomon model, sigma=FepsilonN, and in this paper, Ag-Cu alloys were studied in various contents and heat treatments. Results obtained are as follows [1] Theoretically, the equations should hold between experimental values--epsilonT, ST and calculated values --N, F(F/e)N, that is epsilonT=N, and ST=F(N/e)N. In the case of Ag-Cu alloys, these relations agree well with the theoretical equations. In other words, the shape of true stress-true strain curves for Ag-Cu alloys almost coincide with the theoretical approximate curves, sigma=FepsilonN. [2] Strain hardening exponent N is very dependent on the micro structures of Ag-Cu alloys, but plastic coefficient F is independent of the micro structures. Coefficient F is directly proportional to sigma T. [3] The relationship of F to N can be expressed by equation of F=R(N+1)/NN+1. This equation may be described to be another form of the strain energy equation. Therefore parameter R is dependent on the strain energy. And the plots by computer agreed well with the experimental values.

摘要

牙科金属的力学性能是通过拉伸强度、屈服点、弹性极限、伸长率等数值来估算的。但在将这些数值应用于实际牙科问题时,人们常常发现它们并不足够适用。近年来,电子计算机得到了发展并广泛应用于各个领域,因此作者尝试用计算机分析合金的真应力-真应变曲线模式。均匀塑性变形区域内的流动曲线用霍洛蒙模型表示为σ = Fε^N,在本文中,对不同成分和热处理的银铜合金进行了研究。得到的结果如下:[1] 理论上,实验值——εT、ST与计算值——N、F(F/e)^N之间应满足方程,即εT = N,且ST = F(N/e)^N。对于银铜合金,这些关系与理论方程吻合得很好。换句话说,银铜合金的真应力-真应变曲线形状几乎与理论近似曲线σ = Fε^N重合。[2] 应变硬化指数N非常依赖于银铜合金的微观结构,但塑性系数F与微观结构无关。系数F与σT成正比。[3] F与N的关系可用方程F = R(N + 1)/N^(N + 1)表示。该方程可被描述为应变能方程的另一种形式。因此,参数R取决于应变能。计算机绘制的曲线与实验值吻合得很好。

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