Strain

A. Sutton
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Abstract

A discussion of the continuum approximation is followed by the definition of deformation as a transformation involving changes in separation between points within a continuum. This leads to the mathematical definition of the deformation tensor. The introduction of the displacement vector and its gradient leads to the definition of the strain tensor. The linear elastic strain tensor involves an approximation in which gradients of the displacement vector are assumed to be small. The deformation tensor can be written as the sum of syymetric and antisymmetric parts, the former being the strain tensor. Normal and shear strains are distinguished. Problems set 1 introduces the strain ellipsoid, the invariance of the trace of the strain tensor, proof that the strain tensor satisfies the transformation law of second rank tensors and a general expression for the change in separation of points within a continuum subjected to a homogeneous strain.
应变
在讨论连续统近似之后,将变形定义为涉及连续统内点间分离变化的变换。这就引出了变形张量的数学定义。位移矢量及其梯度的引入引出了应变张量的定义。线性弹性应变张量包含一个近似,其中位移矢量的梯度被假定为很小。变形张量可以写成对称部分和反对称部分的和,前者是应变张量。正常应变和剪切应变是有区别的。问题集1介绍了应变椭球、应变张量轨迹的不变性、应变张量满足二阶张量变换定律的证明以及连续统中受齐次应变作用时点间距变化的一般表达式。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
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