The research on this page is brought to you by Taylor & Francis Knowledge Centers. This collection is automatically generated from our most recent books and journals on this topic.
A general three-dimensional state of stress can be represented as a point with coordinates (σ1, σ2, σ3) in a three-dimensional Cartesian space known as principal stress space (Figure 6.3), in which the coordinate axes are aligned with the principal stress directions. The principal stress space is also sometimes called the Haigh–Westergaard stress space (Mendelson 1968).
The Haigh–Westergaard stress space consists of three mutually perpendicular axes with three principal stresses as positional coordinates, which are used to represent any admissible state of stress in a loaded component (Section 2.10). In this section, we utilize the same space to determine the geometrical representation of yield surfaces when plastic deformation first appears in the component.
Presenting an explicit step-by-step algorithm for lemaitre's ductile damage model with the crack closure effect in tensile-compressive loadings
The stress tensor is simply expressed by the principal stresses in the Haigh-Westergaard stress space as a diagonal matrix to distinguish the tensile and compressive stresses for a multiaxial stressed state: