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Effect of T-Stress and Non-singularity Terms on Stress IntensityFactor of a Crack

机译:T应力和非奇异项对裂纹应力强度因子的影响

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The singular stress field at the crack tip can be presented by the Williams series as σρθλκ∑ σρ(ρ,θ)=n∑k=1 Akρλkσρk(θ) σθ(ρ,θ)=n∑k=1 Akρλkσθk(θ) σρθ(ρ,θ)=n∑k=1 Akρλkσρθk(θ)where the exponent λκis the stress singularity order,σθκ(g=ρ,θρθ)are the associated stress angle functions which represent the stress components in the corresponding directions.Aκ(κ=1,2,1,N)are the associated amplitude coefficients,N is the number of the eigenvalues truncated. In traditional linear fracture mechanics, only the singularity terms corresponding toλκ<0 are take into account in Eq.(1).However, the T-stress term corresponding to λκ=0 and non-singular terms corresponding to λκ>0 at the Williams series expansion play a significant role in determining the stress and strain fields and the energy around the crack tip which in turn can affect the fracture of the specimen predicted by different fracture criteria. But the calculation of the T-stress term and the non-singularity terms in Eq.(1) are very difficult. In this paper, a small rotundity with radius ρis dug out from the tip of the crack. The displacement and stress fields are expressed by Williams series in this small rotundity region. The remaining region is modeled by boundary element method because there is no singularity. By the continuity conditions between the rotundity and the remaining structure, all the unknown values on the boundary and all the Ak in Eq.(1) can be obtained. By this means, the T-stress and the non-singular terms are determined by the boundary element method. Then the effect of the T-stress and the non-singular terms on the calculation of the stress intensity factor of the crack is studied. The results show that the stress intensity factor taking account into the T-stress and the non-singularity terms is more approaching to the experiment results.
机译:裂纹尖端处的奇异应力场可以由Williams级数表示为σρθλκ∑σρ(ρ,θ)= n∑k = 1Akσλkσρk(θ)σθ(ρ,θ)= n∑k = 1Akρλkσθk(θ) σρθ(ρ,θ)= n∑k = 1Akρλkσρθk(θ)其中指数λκ是应力奇异阶,σθκ(g =ρ,θρθ)是相关的应力角函数,代表相应方向上的应力分量。 (κ= 1,2,1,N)是关联的振幅系数,N是被截断的特征值的数量。在传统的线性断裂力学中,方程(1)仅考虑了与λκ<0对应的奇异项,但在Williams处,与λκ= 0对应的T应力项和与λκ> 0对应的非奇异项级数扩展在确定应力场和应变场以及裂纹尖端附近的能量方面起着重要作用,而裂纹尖端周围的能量又会影响通过不同断裂准则预测的试样的断裂。但是等式(1)中的T应力项和非奇异项的计算非常困难。在本文中,从裂纹尖端挖出了一个半径为ρ的小圆度。在这个小圆形区域,位移和应力场用威廉姆斯级数表示。剩余区域通过边界元方法建模,因为没有奇异点。通过圆度和剩余结构之间的连续性条件,可以获得方程(1)中边界上的所有未知值和所有Ak。通过这种方式,通过边界元法确定T应力和非奇异项。然后研究了T应力和非奇异项对裂纹应力强度因子计算的影响。结果表明,考虑到T应力和非奇异项的应力强度因子更接近实验结果。

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