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Impression Creep Behavior of a Cast AZ91 Magnesium Alloy

机译:铸造AZ91镁合金的蠕变蠕变行为

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摘要

The creep behavior of the cast AZ91 magnesium alloy was investigated by impression testing. The tests were carried out under constant punching stress in the range 100 to 650 MPa, corresponding to 0.007 ≤ σ imp/G ≤ 0.044, at temperatures in the range 425 to 570 K. Assuming a power-law relationship between the impression velocity and stress, depending on the testing temperature, stress exponents of 4.2 to 6.0 were obtained. When the experimental creep rates were normalized to the grain size and effective diffusion coefficient, a stress exponent of approximately 5 was obtained, which is in complete agreement with stress exponents determined by the conventional creep testing of the same material reported in the literature. Calculation of the activation energy showed a slight decrease in the activation energy with increasing stress such that the creep-activation energy of 122.9 kJ/mol at σ imp/G = 0.020 decreases to 94.0 kJ/mol at σ imp/G = 0.040. Based on the obtained stress exponents and activation energy data, it is proposed that dislocation climb is the controlling creep mechanism. However, due to the decreasing trend of creep-activation energy with stress, it is suggested that two parallel mechanisms of lattice and pipe-diffusion-controlled dislocation climb are competing. To elucidate the contribution of each mechanism to the overall creep deformation, the creep rates were calculated based on the effective activation energy. This yielded a criterion that showed that, in the high-stress regimes, the experimental activation energies fall in the range in which the operative creep mechanism is dislocation climb controlled by dislocation pipe diffusion. In the low-stress regime, however, the lattice-diffusion dislocation climb is dominant.
机译:通过压痕测试研究了铸造的AZ91镁合金的蠕变行为。该测试是在425至570 K的温度下,在100至650 MPa的恒定冲压应力(相当于0.007≤σimp / G≤0.044)下进行的。压痕速度和应力取决于测试温度,所获得的应力指数为4.2至6.0。当将实验蠕变速率归一化到晶粒尺寸和有效扩散系数时,获得的应力指数约为5,这与文献中报道的相同材料的常规蠕变测试确定的应力指数完全一致。活化能的计算结果表明,活化能随应力的增加而略有下降,使得在σimp / G = 0.020时蠕变活化能为122.9 kJ / mol,在σimp时蠕变活化能降至94.0 kJ / mol /G=0.040。根据获得的应力指数和活化能数据,提出位错爬升是控制蠕变的机制。然而,由于蠕变活化能随应力的下降趋势,提示晶格和管扩散控制的位错爬升的两个平行机制是相互竞争的。为了阐明每种机制对总体蠕变变形的贡献,基于有效激活能计算了蠕变速率。这产生了一个标准,该标准表明,在高应力状态下,实验活化能落在有效蠕变机理是位错管扩散控制位错爬升的范围内。然而,在低应力状态下,晶格扩散位错爬升占主导。

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  • 来源
    《Metallurgical and Materials Transactions A》 |2009年第1期|116-127|共12页
  • 作者

    F. Kabirian; R. Mahmudi;

  • 作者单位

    School of Metallurgical and Materials Engineering University of Tehran Tehran Iran;

    School of Metallurgical and Materials Engineering University of Tehran Tehran Iran;

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  • 正文语种 eng
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