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首页> 外文期刊>Archives of Metallurgy and Materials >THE TENSILE TEST CURVE OF WIRE AFTER ITS CURVATURE CHANGING
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THE TENSILE TEST CURVE OF WIRE AFTER ITS CURVATURE CHANGING

机译:导线弯曲后的拉伸试验曲线

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Stress and strain state during the curvature change are characterized by great non-uniformity. There are circumferential tensile stresses in the external elongated zone and compressive ones in the internal zone. Both zones are separated by the neutral surface where circumferential stresses equal zero. Circumferential strains during curvature change can be determined from: epsilon_(theta) = (x/rho). In the neighbourhood of the neutral surface the material is in the elastic state and the circumferential stresses can be calculated on the basis on equation: sigma_(theta) = (x/rho) centre dot E. Range of the elastic zone can be determined from the condition that the circumferential stresses reach the value of yield stress. ((x_0)/rho) centre dot E = sigma_p. As a result of superimposing of the unloading stresses on the stresses appearing during the active phase of the process some stresses called residual stresses will remain after the process is finished. During tension of a wire having the residual stresses first elastic deformation is observed in the wire, and the tensile force changes linearly depending on the deformation. When sum of the stresses resulting from the external loading and residual stresses reaches the yield stress value, the material is in the plastic condition. With the increase of the stress resulting from the external loading the plastic zone is gradually expanding. In the elastic zone stresses grow proportionally to the strain while in the plastic zone rise in stresses will occur in the range from residual stresses to the yield stress value. Borders between the zones can be determined from the boundary conditions saying that sum of stresses from external loading and residual stresses reaches value of yield stress. On the basis of given equations first distribution of the residual stresses on the cross-section of the wire and then values of forces for the elastic and plastic zones were determined. Considering the peculiarity of the change of stresses in the elastic and plastic zones equations describing tensile force for elastoplastic stage of tension were derived and compared with forces observed in the experiment.
机译:曲率变化过程中的应力和应变状态具有很大的不均匀性。在外部细长区域中有周向拉应力,而在内部区域中有压应力。两个区域都被中性表面隔开,该区域的圆周应力等于零。曲率变化过程中的周向应变可以根据以下公式确定:epsilon_θ=(x / rho)。在中性表面附近,材料处于弹性状态,可以根据以下公式计算周向应力:sigma_θ=(x / rho)中心点E。可以从以下公式确定弹性区域的范围:圆周应力达到屈服应力值的条件。 ((x_0)/ rho)中心点E = sigma_p。由于将卸载应力叠加在过程的有效阶段中出现的应力上,因此在过程完成后将保留一些称为剩余应力的应力。在具有残余应力的金属丝张紧期间,在金属丝中观察到第一弹性变形,并且张力根据变形线性变化。当外部载荷和残余应力所产生的应力之和达到屈服应力值时,材料处于塑性状态。随着外部载荷引起的应力增加,塑料区域逐渐扩大。在弹性区内,应力与应变成比例地增长,而在塑性区内,应力的上升将发生在从残余应力到屈服应力值的范围内。可以根据边界条件确定区域之间的边界,边界条件是外部载荷和残余应力的总和达到屈服应力的值。根据给定的方程,首先在钢丝的横截面上分配残余应力,然后确定弹性和塑性区域的力值。考虑到弹性和塑性区中应力变化的特殊性,推导了描述弹力拉伸阶段拉伸力的方程,并将其与实验中观察到的力进行了比较。

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