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Physics · 术语表

什么是 Traction and the stress tensor?

Definition 3.3 University Physics — Year 3 · 第 3 章 — Continuum Mechanics and Elasticity

Cut the solid, in thought, along a small surface  ⁣dS\dd S of normal n→\vect n: the material on the +n→+\vect n side pulls on the other side with a force  ⁣dF→=σ(n→)  ⁣dS\dd\vect F = \boldsymbol\sigma(\vect n)\,\dd S — the traction. This force depends linearly on n→\vect n (Cauchy), so it is encoded by the stress tensor σij\sigma_{ij}:

 ⁣dFi=∑jσij nj  ⁣dS,\dd F_i = \sum_j \sigma_{ij}\,n_j\,\dd S ,

in pascals. σxx\sigma_{xx} is a pull (>0> 0: tension) or push (<0< 0: compression) across a face normal to xx; σxy\sigma_{xy} is a force along xx carried by a face normal to yy — a shear stress. A fluid at rest is the special case σij=−p δij\sigma_{ij} = -p\,\delta_{ij}: pressure pushes equally on every face and shears on none, which is why fluids flow — they cannot carry static shear.

The three components of the traction on one face of a material cube: one normal (tension or compression), two tangential (shear). The nine components over the three faces form the stress tensor.
The three components of the traction on one face of a material cube: one normal (tension or compression), two tangential (shear). The nine components over the three faces form the stress tensor.
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