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A Method for the Analysis of the Growth of Short Fatigue Cracks

机译:一种分析短疲劳裂缝生长的方法

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The behavior of short fatigue cracks is a matter of importance not only because much of the fatigue lifetime is spent in propagating these cracks, but also because the boundary between propagation and non-propagation separates the safe from the potentially unsafe fatigue regimes. The method of analysis is based upon the following equation: where a is the crack length (in the case of crack starting from a hole, a is taken to be equal to the radius of the hole plus X, the actual length of the crack), N is the number of cycles, A is a material constant, triangle open K_(eff) is the effective value of the stress intensity factor (given by K_(max)-K_(op), where K_(max) is the maximum value of the stress intensity factor in a loading cycle and K_(op) is the crack opening level), and triangle open K_(eff) is the effective value of the stress intensity factor at the threshold level. In order to analyze the crack growth behavior of short fatigue cracks three modifications of Eq. 1 are needed. These are: (1) an elastic-plastic modification because the fatigue strengths are high with respect to the yield strength, (2) a modification to take into account that in the short crack range the fatigue strength rather than the threshold level becomes the dominant factor in affecting fatigue crack growth, and (3) a modification to account for the development of crack closure in the wake of a newly formed fatigue crack. With these modifications Eq. la becomes: where r_c is a material constant of the order of 1 urn in size, F, the elastic-plastic correction factor, equals Y is a geometric factor, triangle sigma is the stress range, k is a material constant which determines the rate of crack closure development, X is the length of a newly formed crack, i.e., the length measured from a free surface or from the root of a notch, and K_(opmax) is the crack opening level for a macroscopic crack. A number of examples will be provided to demonstrate the general applicability of Eq. 2a to situations involving short fatigue crack growth.
机译:的短疲劳裂纹的行为是重要的问题,不仅是因为太多的疲劳寿命的在传播的这些裂纹是花,而且还因为传播和非传播之间的边界分隔开潜在不安全疲劳机制的安全。分析的方法是基于以下等式:其中,a为裂缝长度(在裂缝从孔开始的情况下,一个被取为等于所述孔加X的半径,裂纹的实际长度)中,N是循环的数量,A是材料常数,三角形开放K_(EFF)是应力强度因子的有效值(由K_(最大值)-K_(OP)给出,其中K_(max)为最大在加载循环和K_(OP)的应力强度因子的值是裂纹开口电平),三角形开放K_(EFF)是应力强度因子的阈值电平的有效值。为了分析的短疲劳裂纹等式3个修饰的裂纹增长行为。 1是必要的。它们是:(1)一个弹塑性变形例因为疲劳强度高相对于屈服强度,(2)考虑到的是,在短裂纹范围的疲劳强度,而比阈值电平成为支配的变形例因子对疲劳裂纹增长,和(3)的修改以考虑到裂纹闭合的在一个新形成的疲劳裂纹的唤醒的发展。有了这些修改公式。 LA变为:其中R_C是尺寸为1个瓮的量级的材料常数,F,弹塑性校正因子,等于Y的几何因子,三角形西格玛是应力范围,K是决定速率的材料常数裂纹闭合发展的,X是一个新形成的裂纹,即,从自由表面或从缺口根部测量的长度的长度,和K_(opmax)为宏观裂纹裂纹开口水平。将提供一些实施例以证明式的普遍适用性。图2a涉及短疲劳裂纹增长的情况。

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