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为研究高频谐振式疲劳裂纹扩展试验中带有Ⅰ型预制裂纹的紧凑拉伸(CT)试件裂纹尖端力学参数的变化规律,利用动态有限元方法,采用ANSYS和MATLAB软件编写程序,计算了CT试件在高频恒幅正弦交变载荷作用下,在一个应力循环及裂纹扩展到不同长度时裂纹尖端区域的位移、应变场及裂纹尖端的应力强度因子,并分析了其变化规律。在计算裂纹尖端应力强度因子时,首先采用静态有限元方法和理论公式验证了有限元建模和计算的正确性,然后采用动态有限元方法研究了裂纹扩展过程中裂纹尖端应力强度因子的变化规律。最后进行了高频谐振式疲劳裂纹扩展试验,采用动态高精度应变仪测量了裂纹扩展到不同阶段时裂纹尖端点的应变,并对有限元计算结果进行了验证。研究结果表明:在稳态裂纹扩展阶段,高频谐振载荷作用下Ⅰ型疲劳裂纹尖端位移、应变及应力强度因子均为与载荷同一形式的交变量;随着裂纹的扩展,Ⅰ型疲劳裂纹尖端的位移、应变及应力强度因子幅不断增大;静态应力强度因子有限元计算值和理论值的误差为2.51%,裂纹尖端点应变有限元计算结果和试验结果最大误差为2.93% 。 相似文献
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双材料界面裂纹应力强度因子计算 总被引:1,自引:0,他引:1
建立不同裂纹长度的双材料界面裂纹模型,用有限元软件计算和分析界面裂纹尖端附近的应力场和位移场.利用裂尖前沿应力和裂纹面相对位移分别计算了界面裂纹尖端的应力强度因子K,两种方法计算的K值完全吻合.通过数值分析,给出一种计算双材料界面裂纹应力强度因子K的经验公式. 相似文献
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两种材料的性质对双材料界面裂纹能量释放率及应力强度因子的影响 总被引:3,自引:2,他引:1
在实际工程中,结构往往是由多种材料构成,而裂纹经常在两种材料的界面上扩展.针对双材料界面裂纹,建立相应的计算模型.用能量释放率来描述裂纹的扩展情况,并根据界面裂纹能量释放率解析计算方法对不同的材料性质、外荷载、构件厚度,以及裂纹两侧不同的材料宽度对裂纹扩展时的能量释放率和应力强度因子进行仿真分析,得到了能量释放率和两种材料的弹性模量、外荷载及构件厚度之间的关系变化的曲线,以及裂纹两侧不同的材料宽度和应力强度因子之间的关系.并对界面裂纹和单一材料裂纹的情况进行分析、比较. 相似文献
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T形焊接接头根部裂纹应力强度因子研究 总被引:4,自引:0,他引:4
建立T形焊接接头根部裂纹的半椭圆裂纹模型,定义裂纹模型的构形参数以及边界条件,分析裂纹尖端的应力强度因子。采用奇异单元法,通过有限元计算,模拟裂纹尖端的应力奇异性。并通过收敛性检验确定裂纹尖端的单元尺寸。在此基础上,计算裂纹尖端量纲一应力强度因子,并分析其受几何参数影响的变化规律。计算结果表明,对于给定的载荷条件下,不同初始裂纹尺寸时,裂纹尖端的应力强度因子存在一定的规律性,且不同几何参数对应力强度因子的影响程度存在一定差异,因此,对焊接结构疲劳强度研究时需要有一定的侧重点。采用多重线性回归方法拟合仿真计算结果,这些结果为进一步研究T形焊接接头根部裂纹扩展和疲劳寿命预测提供参考。 相似文献
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裂纹是引起管道开裂失效的主要原因,裂纹尖端应力强度因子是表征裂纹应力场强度的主要物理量,也是对管道进行安全评估时的主要依据之一,但管道不同于平板,有曲率影响,因此基于平板推导出来的裂纹尖端应力强度因子公式必须进行修正。为了准确计算管道上斜裂纹应力强度因子,建立了不同管道直径、不同裂纹倾角以及不同裂纹长度下的管道穿透斜裂纹有限元模型,并计算了裂纹尖端应力强度因子,在无限大板中心斜裂纹应力强度因子计算公式基础上,修正得到了管道穿透斜裂纹应力强度因子计算公式,这对于含裂纹管道安全评定有重要参考价值。 相似文献
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以渐开线直齿轮为研究对象,通过齿轮应力分析确定轮齿裂纹易萌生位置,利用ABAQUS软件建立齿轮裂纹扩展有限元模型,获取齿根裂纹扩展路径,计算不同阶段裂纹尖端应力强度因子.通过多种曲线拟合方式的对比,选取指数函数建立的裂纹长度与裂纹尖端应力强度因子幅之间的函数关系.运用Paris公式构建裂纹扩展速率模型,实现含齿根裂纹齿... 相似文献
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研究了含有裂纹的金属板料在激光冲击波载荷作用下裂纹尖端应力强度因子和裂纹扩展速度的变化,利用断裂力学理论,对激光冲击加载下裂尖参数计算模型进行优化,采用应力强度因子叠加法,将外加载荷引起的应力强度因子和激光冲击后残留的残余压应力引起的应力强度因子叠加,推导出下裂纹尖端应力场强度因子表达式,由此可精确计算出金属板料的裂纹萌生寿命和裂纹扩展速度,实验验证了航空钛合金Ti6Al4V激光冲击后残余应力对裂纹扩展速度的影响,从而建立了激光冲击作用对板料裂纹扩展的影响的理论模型。 相似文献
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Yumin He Junjie Ye Xuefeng Chen Zhengjia He 《Mechanical Systems and Signal Processing》2009,23(3):804-810
The stress intensity factor plays an important role in the calculation of the local flexibility due to the crack in a cracked structure. Many researches on the stress intensity factors in a cracked beam or rotor have been made, but there are some difficulties in calculating the stress intensity factors in a cracked pipe. Maiti et al. obtained the local flexibility due to the crack in a pipe experimentally by deflection and natural frequency methods without calculating the stress intensity factor. In this paper, the stress intensity factor in a cracked pipe can be calculated by dividing a cracked pipe into a series of thin annuli, and a method to calculate the local flexibility due to the crack in a pipe is presented. The experiment results are given to verify the effectiveness of such a method. 相似文献
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基于线性累积损伤理论,分析了含裂纹损伤的加筋板加强筋宽度的不同对裂纹尖端应力强度因子的影响。然后根据分析得到裂纹尖端应力强度因子随加强筋宽度的变化规律。结果表明,随着加强筋宽度的增大,结构应力强度因子的下降幅度逐渐增大,当裂纹尖端离筋条越近时,这种现象越明显。 相似文献
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Jai Hak Park Gennadiy P. Nikishkov 《Journal of Mechanical Science and Technology》2011,25(9):2335-2344
An SGBEM-FEM alternating method had been proposed by Nikishkov, Park and Atluri for the analysis of three-dimensional planar
and non-planar cracks and their growth. The proposed method is an effective method for fatigue or stress corrosion crack growth
simulation. During crack growth simulation, however, an oscillation phenomenon is observed in crack advance or stress intensity
factor distribution. If oscillating amplitude in SIF or crack advance does not decrease during next increment steps, the crack
growth simulation fails. In this paper several methods are examined to remove the oscillation phenomenon. As a result, it
is found that smoothing in stress intensity factor distribution or in crack front geometry can remove or weaken the oscillation
phenomenon. Using the smoothing techniques, stress corrosion crack growth simulation is performed for a semi-elliptical surface
crack and a through-thickness crack embedded in a plate. Crack front shape and stress intensity factor distribution are obtained
after each increment during the crack growth. And the depth and length of a crack are obtained as a function of time. It is
noted that the SGBEM-FEM alternating method is a very effective method for SCC growth simulation for a surface crack and a
through-thickness crack. 相似文献
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A cracked plate with a patch bonded on one side was treated with a crack-bridging model using weight function : assuming continuous
distribution of springs acting between th crack surfaces, the stress intensity factor of the patched crack was numerically
obtained. Especially in the case of a patched crack subjected to residual non-uniform stress, the stress intensity factor
was easily with the corresponding approximate weight function. This paper presented the stress intensity factors for a crack
partially patched within a finite plate or a patched crack initiated from a notch. 相似文献
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为准确计算基于扩展有限元法(XFEM)的裂纹扩展模型中的应力强度因子,在ABAQUS软件中建立中心裂纹平板和三点弯曲的XFEM模型,采用相互作用积分法,通过用户子程序接口分别实现了Ⅰ型、Ⅱ型断裂模式下裂纹扩展过程中应力强度因子的计算;研究了网格密度与积分半径对XFEM模型应力强度因子计算精度的影响规律,研究结果表明:当网格密度因子为0.012~0.016、相对积分半径为3时,应力强度因子收敛至稳定值,计算误差不超过3%。利用所提方法与程序计算了单边带孔疲劳裂纹扩展试样的动态应力强度因子,试验结果表明:基于Paris理论预测的剩余寿命与疲劳试验结果误差为5.3%,进一步验证了所提方法与程序的正确性。 相似文献
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高速列车锻钢制动盘热疲劳裂纹耦合扩展特性研究 总被引:5,自引:1,他引:5
据制动盘裂纹剖面的宏观形貌,发现盘面长裂纹的形成以多条半椭圆表面裂纹连通为主。针对制动盘在运行过程中的典型运用工况,采用有限元法计算制动盘在300 km/h紧急制动后的热应力,发现周向残余应力较大,并以此推测周向残余应力是驱动制动盘热疲劳裂纹扩展的主要原因。在此基础上,建立制动盘盘面的裂纹网格,研究了裂纹扩展过程中的应力强度因子和多裂纹耦合扩展规律。通过研究发现对于给定的载荷条件,不同初始形状比时,裂纹前缘应力强度因子的分布规律存在一定的规律性,随着裂纹的扩展,裂纹形状趋于扁平化;多裂纹扩展时,裂纹间距越小,裂纹间的相互作用越明显,扩展速度越快;但受制动盘结构和尺寸限制,共线裂纹数越多,每条裂纹扩展到临界值时的应力强度因子越小。 相似文献
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《Wear》1996,199(1):9-23
A linear elastic fracture mechanics analysis of plane-strain indentation of a homogeneous half-space with a subsurface horizontal crack was performed using the finite element method. Stress intensity factor results obtained for an infinite plate with a central crack subjected to far-field tension and a half-space with a frictionless subsurface horizontal crack under a moving surface point load are shown to be in good agreement with corresponding analytical results. Crack mechanism maps illustrating the occurrence of separation, forward and backward slip, stick, and separation at the crack interface are presented for different indentation load positions and crack face friction coefficients. Results for the stresses in the vicinity of the crack tips and the mode I and mode II stress intensity factors are given for different indentation positions, crack face friction coefficients, and both concentrated and distributed surface normal tractions. Although indentation produces a predominantly shear and compressive stress field, mode I loading conditions are shown to occur for certain indentation positions. However, the magnitude of the mode I stress intensity factor is significantly smaller than that of mode II, suggesting that in-plane shear mode crack growth is most likely to occur in the absence of microstructural defects. The significance of crack face friction and sharpness of the indenter on the subsurface shear mode crack propagation rate is interpreted in terms of the mode II stress intensity factor range and material behavior. 相似文献