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首页> 外文期刊>International Journal of Solids and Structures >Strain gradient solution for a finite-domain Eshelby-type plane strain inclusion problem and Eshelby's tensor for a cylindrical inclusion in a finite elastic matrix
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Strain gradient solution for a finite-domain Eshelby-type plane strain inclusion problem and Eshelby's tensor for a cylindrical inclusion in a finite elastic matrix

机译:有限域Eshelby型平面应变夹杂问题的应变梯度解和有限弹性矩阵中圆柱夹杂的Eshelby张量

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A solution for the finite-domain Eshelby-type inclusion problem of a finite elastic body containing a plane strain inclusion prescribed with a uniform eigenstrain and a uniform eigenstrain gradient is derived in a general form using a simplified strain gradient elasticity theory (SSGET). The formulation is facilitated by an extended Betti's reciprocal theorem and an extended Somigliana's identity based on the SSGET and suitable for plane strain problems. The disturbed displacement field is obtained in terms of the SSGET-based Green's function for an infinite plane strain elastic body, which differs from that in earlier studies using the three-dimensional Green's function. The solution reduces to that of the infinite-domain inclusion problem when the boundary effect is suppressed. The problem of a cylindrical inclusion embedded concentrically in a finite plane strain cylindrical elastic matrix of an enhanced continuum is analytically solved for the first time by applying the general solution, with the Eshelby tensor and its average over the circular cross section of the inclusion obtained in closed forms. This Eshelby tensor, being dependent on the position, inclusion size, matrix size, and a material length scale parameter, captures the inclusion size and boundary effects, unlike existing ones. It reduces to the classical elasticity-based Eshelby tensor for the cylindrical inclusion in an infinite matrix if both the strain gradient and boundary effects are not considered. Numerical results quantitatively show that the inclusion size effect can be quite large when the inclusion is very small and that the boundary effect can dominate when the inclusion volume fraction is very high. However, the inclusion size effect is diminishing with the increase of the inclusion size, and the boundary effect is vanishing as the inclusion volume fraction becomes sufficiently low.
机译:使用简化的应变梯度弹性理论(SSGET),以一般形式导出了包含平面应变夹杂物的有限弹性体的有限域Eshelby型夹杂问题的解决方案,该平面应变夹杂物具有均一的本征应变和均一的本征应变梯度。扩展的Betti倒数定理和基于SSGET的扩展的Somigliana身份简化了该公式,并且适用于平面应变问题。扰动位移场是根据无限平面应变弹性体基于SSGET的格林函数获得的,这与早期使用三维格林函数的研究有所不同。当边界效应被抑制时,该解决方案简化为无限域包含问题。同轴地嵌入增强连续体的有限平面应变圆柱弹性矩阵中的圆柱夹杂问题首次通过应用广义解进行了分析求解,并使用Eshelby张量及其在夹杂物的圆形截面上的平均值求出。封闭表格。该Eshelby张量取决于位置,夹杂物大小,矩阵大小和材料长度比例参数,可捕获夹杂物大小和边界效应,这与现有的不同。如果没有同时考虑应变梯度和边界效应,则可以简化为无限大矩阵中的圆柱包含的基于弹性的经典Eshelby张量。数值结果定量地表明,当夹杂物非常小时,夹杂物尺寸效应会非常大;当夹杂物体积分数非常高时,边界效应将占主导地位。然而,随着夹杂物尺寸的增加,夹杂物尺寸效应减小,并且随着夹杂物体积分数变得足够低,边界效应消失。

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