(7.15)
Section 7.7
Furthermore, it is occasionally more convenient to represent strain as true strain T, defined by
(7.16)
If no volume change occurs during deformation, that is, if
前面内容 总结复习
固体中的原子有序 (Perfections in Solids) 固体中的原子无序 (Imperfections in Solids) 固体中的转变 (Transformations in Solids) 固体物质的表面结构 (Surface Structures of Solid Materials)
A standard tensile specimen
23
Sometimes it is more meaningful to use a true stress–true strain scheme. True stress T is defined as the load F divided by the instantaneous cross-sectional area Ai over which deformation is occurring (i.e., the neck, past the tensile point), or
Ai li = A0l0
(7.17)
true and engineering stress and strain are related according to
(7.18a) (7.18b)
Equations 7.18a and 7.18b are valid only to the onset of necking; beyond this point