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Erratum to: Closure of circular arc cracks under general loading: effects on stress intensity factors

机译:勘误至:在一般载荷下闭合圆弧裂纹:对应力强度因子的影响

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Due to an unfortunate turn of events, this article has been published with an erroneous version of Fig. 6 and two errors in the values of the second paragraph as well as one error in the text of paragraph three of Sect. 5 "Arc crack closure under uniaxial tension". Please find below the correct values and text part of the second and third paragraph of Sect. 5 and the correct Fig. 6 that should be regarded by the reader as the final versions.Figure 6 shows displacement fields normalized by the magnitude of the maximum displacement within that field. The initial and exaggerated final crack geometries are also shown in Fig. 6 in order to illustrate the deformation of the crack surfaces. Note that in general, displacements within the concavity of the arc crack have greater magnitudes than those in the surrounding material. Although the displacement fields in Fig. 6 are plotted with similar vector lengths, the magnitude of the maximum displacement differs both with arc crack half-angle α and loading orientation co. In comparing the examples of arc cracks with a = 45° and α = 90°, the lesser half angle yields lesser displacement discontinuities. For all arc crack half angles, as ω increases and the direction of uniaxial tension becomes more parallel to the arc crack chord, the magnitude of maximum displacement decreases. As the loading orientation ω increases from 0° to 90°, the maximum displacement discontinuity magnitude plotted decreases 80.6 and 58.0% for arc cracks with α = 45° and α = 90°, respectfully. Additionally, the rate of change of the maximum magnitude increases as the loading orientation co increases from 0° to 90°.
机译:由于不幸的事件发生,本文已发表,并带有错误的图6版本以及第二段的值中的两个错误以及Sect第三段的文本中的一个错误。 5“单轴张力下的电弧裂纹闭合”。请在下面找到该节第二段和第三段的正确值和文本部分。 5和正确的图6应该被读者视为最终版本。图6显示了位移场,该场通过该场内最大位移的大小进行了归一化。初始和夸张的最终裂纹几何形状也显示在图6中,以说明裂纹表面的变形。请注意,通常,电弧裂纹的凹部内的位移的大小要比周围材料中的大。尽管图6中的位移场是用相似的矢量长度绘制的,但最大位移的大小随电弧裂纹半角α和载荷方向co的不同而不同。在比较a = 45°和α= 90°的电弧裂纹的示例时,较小的半角产生的位移不连续性较小。对于所有电弧裂纹半角,随着ω的增加和单轴拉伸方向变得与电弧裂纹弦更平行,最大位移的幅度减小。当载荷方向ω从0°增加到90°时,对于α= 45°和α= 90°的电弧裂纹,绘制的最大位移不连续量分别减少了80.6%和58.0%。此外,最大强度的变化率随着加载方向co从0°增加到90°而增加。

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