Differentiation of the elastic stress-strain relations (4.8) and the discrete flow rule (4.9) yields
Combining this two equations, one obtains following relation
where
![$ \Xi$](img502.png)
is the algorithmic moduli defined as
![$\displaystyle \mbox{\boldmath$\Xi$}$](img500.png) ![$\displaystyle _{n+1}=\left[\mbox{\boldmath$D$}^{-1}+\sum\lambda^i\partial_{\sig...
...\lambda\partial_{\sigma\kappa}g\partial_{\sigma}\mbox{\boldmath$\kappa$}\right]$](img503.png) |
(4.27) |
Differentiation of discrete consistency condition yields
By substitution of (4.26) into (4.28) the following relation is obtained
where matrix
is defined as
![$\displaystyle \mbox{\boldmath$G$}$](img384.png) ![$\displaystyle =\left[\mbox{\boldmath$V$}^T\mbox{\boldmath$\Xi$}\mbox{\boldmath$...
...kappa}\mbox{\boldmath$f$}\partial_{\lambda}\mbox{\boldmath$\kappa$}\right]^{-1}$](img510.png) |
(4.30) |
Finally, by substitution of (4.30) into (4.26) one obtains the algorithmic elastoplastic tangent moduli
Borek Patzak
2017-12-30