Determination of the Elastic Tensor of a Textured Low-Carbon Steel

P. Spalthoff, W. Wunnike, C. Nauer-Gerhard, H. Bunge, E. Schneider
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引用次数: 12

Abstract

The components of the elastic stiffness tensor of hot rolled low-carbon steel were determined using an ultrasonic pulse-echo-method. They were also calculated on the basis of X-ray texture measurements using the Hill approximation. The maximum deviation between experimental and calculated values is 3.5%. An influence of the slightly anisotropic grain structure on the elastic anisotropy could not be seen. and position of each crystallite is known, then the boundary conditions in the grain boundaries can be strictly taken into account and the polycrystal properties can be calculated straight foreward. However, this is usually not the case. Certain statistical assumptions must then be made which lead to various approximative models for the polycrystal constants. In the Reuss model (Reuss, 1929), constant stress is assumed whereas the Voigt model (Voigt, 1928) assumes constant strain throughout the polycrystal. The polycrystal constants are then the simple volume averages of the components of the stiffness and compliance tensor of the individual crystallites, respectively. These assumptions are limiting cases, the actual values must lie between them. In a first approximation, knowing nothing about the microstructure, the average of both these assumptions can be taken, corresponding to the Hill approximation (Hill, 1952). It has been found that this approximation, although theoretically unsatisfactory, agrees with the experimen- tal results within a few percent, which is sufficient for most practical purposes. A theoretically much more satisfactory model was developed by Kr6ner (Kr6ner, 1958). In this model a spherical grain is embedded in a polycrystalline matrix
织构低碳钢弹性张量的测定
采用超声脉冲回波法测定了热轧低碳钢弹性刚度张量的分量。它们也是在使用Hill近似的x射线纹理测量的基础上计算的。实验值与计算值的最大偏差为3.5%。未观察到微各向异性晶粒结构对弹性各向异性的影响。并且知道了各个晶的位置,就可以严格考虑晶界中的边界条件,从而可以直接计算出多晶的性质。然而,通常情况并非如此。然后必须作出某些统计假设,从而得出多晶体常数的各种近似模型。在Reuss模型(Reuss, 1929)中,假设恒定的应力,而Voigt模型(Voigt, 1928)假设整个多晶体的恒定应变。多晶常数分别是单个晶的刚度张量和柔度张量分量的简单体积平均值。这些假设是极限情况,实际值必须介于它们之间。在第一近似中,对微观结构一无所知,可以取这两个假设的平均值,对应于Hill近似(Hill, 1952)。人们发现,这种近似虽然在理论上不能令人满意,但与实验结果在百分之几以内是一致的,这对于大多数实际目的来说是足够的。Kr6ner (Kr6ner, 1958)提出了一个理论上更令人满意的模型。在这个模型中,球形颗粒嵌入在多晶基体中
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