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Subsonic semi-infinite crack with a finite friction zone in a bimaterial

机译:双材料中具有有限摩擦区的亚音速半无限裂纹

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Propagation of a semi-infinite crack along the interface between an elastic half-plane and a rigid half-plane is analyzed. The crack advances at constant subsonic speed. It is assumed that, ahead of the crack, there is a finite segment where the conditions of Coulomb friction law are satisfied. The contact zone of unknown a priori length propagates with the same speed as the crack. The problem reduces to a vector Riemann-Hilbert problem with a piece-wise constant matrix coefficient discontinuous at three points, 0, 1, and ∞. The problem is solved exactly in terms of Kummer's solutions of the associated hypergeometric differential equation. Numerical results are reported for the length of the contact friction zone, the stress singularity factor, the normal displacement u_2, and the dynamic energy release rate G. It is found that in the case of frictionless contact for both the sub-Rayleigh and super-Rayleigh regimes, G is positive and the stress intensity factor K_(II) does not vanish. In the sub-Rayleigh case, the normal displacement is positive everywhere in the opening zone. In the super-Rayleigh regime, there is a small neighborhood of the ending point of the open zone where the normal displacement is negative.
机译:分析了沿弹性半平面和刚性半平面之间的界面的半无限裂纹的传播。裂纹以恒定的亚音速前进。假定在裂纹之前,存在一个满足库仑摩擦定律条件的有限段。先验长度未知的接触区以与裂纹相同的速度传播。该问题简化为向量Riemann-Hilbert问题,其中分段常数矩阵系数在三个点0、1和∞处不连续。该问题已根据相关超几何微分方程的Kummer解精确解决。报道了接触摩擦区域的长度,应力奇异性因子,法向位移u_2和动能释放速率G的数值结果。发现在无摩擦接触的情况下,子瑞利和超级瑞利都瑞利体制,G为正,应力强度因子K_(II)不消失。在次瑞利情况下,在开口区域中的每个位置的法向位移都是正的。在超级瑞利体制中,法向位移为负的开放区域终点附近有一个很小的区域。

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