剪切波作用下界面裂纹行为的非线性问题

A. V. Menshykov, V. Menshykov, O. Kladova
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引用次数: 0

摘要

给出了谐波剪切波作用下界面裂纹问题的解法。结果表明,其他作者在没有考虑裂纹面接触的情况下进行了相同问题的求解,得到的结果表明,裂纹面是相互贯通的,这是不可能的。从而证明了该问题是非线性的,因为在加载过程中接触区的位置和大小是未知的和可变的。采用边界积分方程法求解,考虑了裂纹面的接触相互作用,利用Somigliana动力恒等式及其导出的边界方程,实现了二维问题向边界等效问题的过渡;边界积分方程中的矢量分量采用傅里叶级数表示,为了防止裂纹面相互渗透和接触区出现拉力,引入了sigorini单边约束。数值求解采用边界元法,在单元上对问题参数进行常数逼近。数值研究了剪切波频率对裂隙面及相邻面位移、裂隙面接触区开度及范围的影响。给出了最大切向分量和法向分量与裂纹面位移之间的定量差异。结果表明,接触区域的位置和长度在加载期间发生变化,接触力的大小沿裂纹长度变化。
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NONLINEAR PROBLEM OF INTERFACE CRACK BEHAVIOR UNDER THE ACTION OF SHEARING WAVE
Solution of the problem for an interface crack under the action of a harmonic shear wave is presented. It is shown that the same problems solutions of other authors were performed without taking into account the crack faces contact, and results obtained indicate the interpenetration of the faces, that is not possible. Thus, it is proved that the problem is nonlinear because the positions and sizes of the contact zone are unknown and variable during the loading. The solution is obtained by the boundary integral equations method taking into account the contact interaction of the crack faces: using the Somigliana dynamic identity and the boundary equations arising from them, the transition from the two-dimensional problem to the equivalent problem at the boundaries of the domain is realized; the vector components in the boundary integral equations are presented by Fourier series, to prevent the interpenetration of the crack faces and the emergence of tensile forces in the contact zone the Signorini unilateral constraints are involved. The numerical solution is performed by the method of boundary elements with constant approximation of the problem parameters on an element. Numerical researches of the shear wave frequency influence onto the crack faces and adjoining surface displacements, opening and extent of crack faces contact zone are carried out. The quantitative difference between the maximum tangential and normal components of adhesion line and the crack faces displacements is shown. It is shown that the position and length of the contact area change during the load period, and the magnitudes of the contact forces vary along the crack length.
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