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Effect of crack shape, inclination angle, and friction coefficient in crack surface contact problems

机译:裂纹形状,倾角和摩擦系数对裂纹表面接触问题的影响

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In rolling/sliding contact fatigue, it is known that the crack propagates at a characteristic angle #theta# = 15-30 deg to the surface. To analyze the mechanism, however, the body force method has been widely used assuming 3D crack models for #theta# = 45-90. In this study, therefore, the unknown body force densities are newly approximated by using fundamental density functions and polynomials. Then, a semi-elliptical crack model is analyzed for #theta# = 15-90 under compressive residual stresses and Hertzian contact loads. The stress intensity factors K_(II), K_(III) are calculated with varying the crack shape b/a, inclination crack angle #theta#, and crack face friction coefficient #mu#. The calculations show that the present method is useful for the analysis for #theta# = 15-30 deg with high accuracy. It is seen that the K_(II)-values when b/a -> 0 are larger than the ones when b/a -> 1 by 0-24 percent for both under compressive residual stress and Hertzian contact load. Regarding the maximum K_(II) values under Hertzian contact load, the results of #theta#=15 deg are smaller than the ones of #theta# =45 deg by 23-34 percent. Regarding the amplitude of (K_(II max) - K_(II min)), the results of #theta# = 15 deg are smaller than the ones of #theta# = 45 deg by 4-24 percent. With increasing the value of friction coefficient #mu# for crack faces the value of K_(II) decreases significantly. When the crack is short and the inclination angle #theta# is small, the value of friction coefficient f for Hertzian contact load largely affect the K_(II) value.
机译:在滚动/滑动接触疲劳中,已知裂纹以特征角度#theta#= 15-30度向表面传播。但是,为了分析其机理,假定#theta#= 45-90的3D裂纹模型,体力法已被广泛使用。因此,在这项研究中,未知的体力密度通过使用基本密度函数和多项式重新近似。然后,在压缩残余应力和赫兹接触载荷下,分析半椭圆裂纹模型的#theta#= 15-90。通过改变裂纹形状b / a,倾斜裂纹角度#θ#和裂纹面摩擦系数#mu#来计算应力强度因子K_(II),K_(III)。计算表明,本方法可用于#theta#= 15-30度的高精度分析。可以看出,在压缩残余应力和赫兹接触载荷下,b / a-> 0时的K_(II)值比b / a-> 1时的K_(II)值大0-24%。关于赫兹接触载荷下的最大K_(II)值,#theta#= 15度的结果比#theta#= 45度的结果小23-34%。关于(K_(II max)-K_(II min))的幅度,#theta#= 15度的结果比#theta#= 45度的结果小4-24%。随着裂纹表面的摩擦系数#mu#值的增加,K_(II)的值显着降低。当裂纹短且倾斜角#θ#小时,赫兹接触载荷的摩擦系数f的值极大地影响K_(II)值。

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