张力场理论

D. Steigmann
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引用次数: 309

摘要

提出了一种用于分析各向同性弹性膜在有限变形下起皱的一般张力场理论。主要贡献是一个描述张力轨迹几何性质的偏微分方程。这是一个由两个方程组成的系统之一,它描述了与变形无关的应力状态。该系统在任何稳定解下都是强椭圆型的,而变形则用抛物线型系统来描述。得到了可控解,即在任何各向同性弹性材料中,仅通过施加边缘牵引力和侧压力就能保持的状态。对一般轴对称问题进行了隐式求解,并将该理论应用于两个典型实例的求解。现有的小应变理论对应于一般理论的奇异极限,在此极限下底层系统由椭圆型变为抛物线型。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
Tension-field theory
A general theory of the tension field is developed for application to the analysis of wrinkling in isotropic elastic membranes undergoing finite deformations. The principal contribution is a partial differential equation describing a geometrical property of tension trajectories. This is one of a system of two equations which describes the state of stress independently of the deformation. This system is strongly elliptic at any stable solution, whereas the deformation is described by a system of parabolic type. Controllable solutions, i. e. those states that can be maintained in any isotropic elastic material by application of edge tractions and lateral pressure alone, are obtained. The general axisymmetric problem is solved implicitly and the theory is applied to the solution of two representative examples. Existing small strain theories are shown to correspond to a singular limit of the general theory, at which the underlying system changes from elliptic to parabolic type.
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