1. Reference problem#

1.1. Geometry#

The stresses and deformations are homogeneous in the volume element. This can be represented by a plane or a solid element, for example:

_images/1000058200000FB600000CD1EFC9375AA8655098.svg

1.2. Material properties#

Law of elastoplastic behavior with linear kinematic work hardening.

_images/1000000000000120000000C1F5BD7A98ED2AF70B.png

\(\begin{array}{c}E\mathrm{=}195000\mathit{MPa}\\ \nu \mathrm{=}0.3\\ {\sigma }^{Y}\mathrm{=}181\mathit{MPa}\\ {E}_{T}\mathrm{=}1930\mathit{MPa}\end{array}\)

1.3. Boundary conditions and loads#

The volume element is locked along \(\mathrm{Ox}\) along the \([\mathrm{2,4}]\) side while being subjected to a pull \({\sigma }^{D}\) and a shear force \({\tau }^{D}\).

_images/10000C960000110E00000B93C8C5FAB7DA58B9F8.svg

The loading path is as follows:

\({\sigma }^{D}\)

\({\tau }^{D}\)

_images/1000000000000125000000B7625D352B37DA2858.png

(\(\mathit{MPa}\))

(\(\mathit{MPa}\))

\(A\)

151.2

93.1

\(B\)

257.3

33.1

\(C\)

259.3

0