几何非线性形式下管道贯通裂纹SIF和COA的有限元计算

A. Oryniak, I. Orynyak
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引用次数: 0

摘要

在对核电站管道系统进行“先漏后破”分析时,应力强度因子(SIF)和裂纹张开面积或位移(COA或COD)的确定是重要的组成部分。其计算的表化参数结果在现代科学和规范文献中广泛出现。然而,有一个方面的裂纹行为,至少在薄壁管道,仍然没有得到应有的重视。我们这里指的是几何非线性效应,它可以大到足以在实际应用中得到解释。在几何线性分析中,认为只有内压才能使裂纹开裂,COA和SIF与之成正比。SIF通常表示为无限大板的解乘以所谓的胀形因子BF,它取决于无因次裂纹长度,即裂纹长度除以半径R与壁厚t乘积的平方根的比率。薄壁管道中的两个载荷因素会导致几何非线性行为。第一类是由轴向力或弯矩值引起的轴向应力。第二,是内心的压力。本文重点讨论了轴向力的影响。为此,建立了具有不同R/t比(20、30、40、50)和不同无因次裂纹长度(2、4、6、8)的管道的数值模型。为了排除由于周向应力引起的非线性,管内压力保持为非常小的值,并且计算了轴向力的无因次SIF和COD值。为了证明所选择的有限元类型、网格划分、单元数沿厚度、加载步骤的正确性,考虑了横向梁在很大轴向力附加作用下的非线性建模辅助问题。达到了很好的通信。对于含轴向裂纹的管道,通过与已有的线性计算结果的比较,对数值模型进行了细致的验证。所得结果以线性和非线性结果之间的差异百分比表示。结果表明,几何非线性的影响在实际应用中是相当重要的,可以达到近3-10%的实际情况。不同轴向应力水平和不同裂纹长度下,几何非线性导致的SIF百分比变化可以很好地表现为应力积、半径厚度比和无因次裂纹长度平方根的独特依赖关系。裂纹中心点的COD变化略大于SIF,除了小裂纹λ < 3外,COD与SIF具有相同的惟一依赖关系。
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FEM Calculations of SIF and COA for Through Axial Cracks in Pipes in Geometrically Nonlinear Formulation
The determination of stress intensity factors (SIF) and crack opening area or displacements (COA or COD) is important constituent when performing the “leak before break” analysis of piping systems in NPPs. The tabulated parametrical results of their calculation are widely presented in modern scientific and normative literature. Nevertheless, there is one aspect of crack behavior, at least in thin walled pipes, which still had not obtained its due attention. We mean here the geometrically nonlinear effect, which can be the big enough to be accounted for in practical applications. It is considered in geometrically linear analysis that only the inner pressure opens the crack, and COA and SIF are directly proportional to it. SIF is presented usually as solution for infinite plate multiplied by so-called bulging factor, BF, which depends on dimensionless crack length, i.e. ratio of crack length divided on square root of product of radius, R, and wall thickness, t. Two loading factors in thin walled pipes can contribute to geometrically nonlinear behavior. The first one is axial stresses induced by value of axial force or bending moment. The second one – is the inner pressure itself. The most attention in present paper is given to influence of the axial force. With this goal the numerical models were created for pipes with different ratios of R/t (20, 30, 40, 50) and different dimensionless crack length (2, 4, 6, 8). To exclude the nonlinearity due to circumferential stress the inner pressure is kept as a very small value and dimensionless SIF and COD values are calculated with respect to axial force. To prove the correctness of choosing the finite element types, meshing, number of elements along the thickness, loading steps the auxiliary problem of nonlinear modeling of transverse beam loaded additionally by very big axial force is considered. The very good correspondence was attained. For the pipe with axial crack the careful verification of numerical model was performed by comparison with linear results existing in literature. The results obtained are presented as a percentage of difference between the linear and nonlinear results. They show that influence of geometrical nonlinearity is fairly essential to be accounted in practice and can reach for practically real cases almost 3–10%. The change of SIF in percentages due to geometrical nonlinearity for different axial stress levels and for different crack lengths can be fairly well presented as unique dependence from product of stresses, radius to thickness ratio, and square root of dimensionless crack length. The change COD in central point of crack is slightly bigger than for SIF and the same unique dependence can be formulated for COD with only exception for small cracks λ < 3.
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