arXivDaily arXiv每日学术速递 周一至周五更新
arXiv 1903.03067cond-mat.mtrl-sci
收藏

点缺陷的非奇异连续介质双Helmholtz型梯度弹性理论

A non-singular continuum theory of point defects using gradient elasticity of bi-Helmholtz type

Markus Lazar

摘要:

在本文中,我们发展了一个非奇异连续理论的点缺陷的基础上的第二应变梯度弹性理论,所谓的梯度弹性bi-Helmholtz型。这种广义连续统理论具有两个内部材料长度的弱非局部特征,并提供了无奇异性的缺陷力学。双Helmholtz型梯度弹性力学基于高阶偏微分方程给出了缺陷的经典奇异性的自然和物理正则化。将各向同性固体中的点缺陷视为双Helmholtz型梯度弹性中的本征应变问题。提出了点缺陷的无奇性场。位移场以及第一,第二和第三梯度的位移导出,它表明,经典奇点在这个框架中进行正则化。该模型给出了位移场、第一位移梯度和第二位移梯度的非奇异表达式。此外,塑性变形(特征变形)和塑性变形的梯度的扩张中心也是非奇异的,并给出了一个形状因子(形状函数)的一个点缺陷。给出了刃型位错应力场中两个膨胀中心之间的相互作用能和相互作用力以及膨胀中心的相互作用能和相互作用力的无奇性表达式。并将所得结果应用于计算膨胀中心的有限自能。

英文摘要:

In this paper, we develop a non-singular continuum theory of point defects based on a second strain gradient elasticity theory, the so-called gradient elasticity of bi-Helmholtz type. Such a generalized continuum theory possesses a weak nonlocal character with two internal material lengths and provides a mechanics of defects without singularities. Gradient elasticity of bi-Helmholtz type gives a natural and physical regularization of the classical singularities of defects, based on higher order partial differential equations. Point defects embedded in an isotropic solid are considered as eigenstrain problem in gradient elasticity of bi-Helmholtz type. Singularity-free fields of point defects are presented. The displacement field as well as the first, the second and the third gradients of the displacement are derived and it is shown that the classical singularities are regularized in this framework. This model delivers non-singular expressions for the displacement field, the first displacement gradient and the second displacement gradient. Moreover, the plastic distortion (eigendistortion) and the gradient of the plastic distortion of a dilatation centre are also non-singular and are given in terms of a form factor (shape function) of a point defect. Singularity-free expressions for the interaction energy and the interaction force between two dilatation centres and for the interaction energy and the interaction force of a dilatation centre in the stress field of an edge dislocation are given. The results are applied to calculate the finite self-energy of a dilatation centre.

机构、总结、中文摘要均由AI分析而来,可能存在错误,请以论文正文为准。

↑